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xmlns:dc="http://purl.org/dc/elements/1.1/">2013-06-15T00:00:00-05:00</dc:date><prism:coverDisplayDate xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">15 June 2013</prism:coverDisplayDate><prism:volume xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">34</prism:volume><prism:number xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">16</prism:number><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1363</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1437</prism:endingPage><image rdf:resource="http://onlinelibrary.wiley.com/store/10.1002/jcc.v34.16/asset/cover.gif?v=1&amp;s=93fb1ad526cd7f7b43abc7bfa505efba0738538d"/><items><rdf:Seq><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23326"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23321"/><rdf:li 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rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23266"/></rdf:Seq></items></channel><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23326" xmlns="http://purl.org/rss/1.0/"><title>Low cost prediction of relative stabilities of hydrogen bonded complexes from atomic multipole moments for overly short intermolecular distances</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23326</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Low cost prediction of relative stabilities of hydrogen bonded complexes from atomic multipole moments for overly short intermolecular distances</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Wiktor Beker, Karol M. Langner, Edyta Dyguda-Kazimierowicz, Mikołaj Feliks, W. Andrzej Sokalski</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-21T09:40:46.415594-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23326</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23326</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23326</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Rapid Communication</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The relative stability of biologically relevant, hydrogen bonded complexes with shortened distances can be assessed at low cost by the electrostatic multipole term alone more successfully than by <em>ab initio</em> methods. These results imply that atomic multipole moments may help improve ligand–receptor ranking predictions, particularly in cases where accurate structural data are not available. © 2013 Wiley Periodicals, Inc.</p></div>
<a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/jcc.23326/asset/image_m/jcc23326-toc-0001-m.png?v=1&amp;s=03fe2b8bf31905348aa52bdfcb845150b5bc18a3" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23326/asset/image_n/jcc23326-toc-0001.png?v=1&amp;s=467a9ffd3663c98b8b18ef933a970bdf5ff753c0"/></a>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>The relative stability of biologically relevant hydrogen bonded complexes with shortened distances can be better assessed by electrostatic multipole interactions than by <em>ab initio</em> methods.
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The relative stability of biologically relevant, hydrogen bonded complexes with shortened distances can be assessed at low cost by the electrostatic multipole term alone more successfully than by ab initio methods. These results imply that atomic multipole moments may help improve ligand–receptor ranking predictions, particularly in cases where accurate structural data are not available. © 2013 Wiley Periodicals, Inc.
The relative stability of biologically relevant hydrogen bonded complexes with shortened distances can be better assessed by electrostatic multipole interactions than by ab initio methods.






</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23321" xmlns="http://purl.org/rss/1.0/"><title>Reply to the comment of Dr. S. Rayne on “QSAR model reproducibility and applicability: A case study of rate constants of oh radical reaction models applied to PBDEs and (B-)TAZs”</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23321</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Reply to the comment of Dr. S. Rayne on “QSAR model reproducibility and applicability: A case study of rate constants of oh radical reaction models applied to PBDEs and (B-)TAZs”</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Paola Gramatica, Simona Kovarich, Partha Pratim Roy</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-21T09:39:31.5266-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23321</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23321</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23321</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Letter to the Editor</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>We appreciate the interest of Dr. Rayne on our article and we completely agree that the dataset of (benzo-)triazoles, which were screened by the hydroxyl radical reaction quantitative structure-activity relationship (QSAR) model,<a href="#jcc23321-bib-0001" rel="references:#jcc23321-bib-0001"/> was not only composed of benzo-triazoles but also included some simpler triazoles (without the condensed benzene ring), such as the chemicals listed by Dr. Rayne, as well as some related heterocycles (also few not aromatic). We want to clarify that in this article<a href="#jcc23321-bib-0001" rel="references:#jcc23321-bib-0001"/> (as well as in other articles<a href="#jcc23321-bib-0002" rel="references:#jcc23321-bib-0002 #jcc23321-bib-0003 #jcc23321-bib-0004 #jcc23321-bib-0005"/> in which the same dataset was screened), for conciseness, the abbreviations (B)TAZs and BTAZs were used as general (and certainly too simplified) notations meaning an extended dataset of benzo-triazoles, triazoles, and related compounds. © 2013 Wiley Periodicals, Inc.</p></div>
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We appreciate the interest of Dr. Rayne on our article and we completely agree that the dataset of (benzo-)triazoles, which were screened by the hydroxyl radical reaction quantitative structure-activity relationship (QSAR) model, was not only composed of benzo-triazoles but also included some simpler triazoles (without the condensed benzene ring), such as the chemicals listed by Dr. Rayne, as well as some related heterocycles (also few not aromatic). We want to clarify that in this article (as well as in other articles in which the same dataset was screened), for conciseness, the abbreviations (B)TAZs and BTAZs were used as general (and certainly too simplified) notations meaning an extended dataset of benzo-triazoles, triazoles, and related compounds. © 2013 Wiley Periodicals, Inc.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23304" xmlns="http://purl.org/rss/1.0/"><title>DOT2: Macromolecular docking with improved biophysical models</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23304</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">DOT2: Macromolecular docking with improved biophysical models</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Victoria A. Roberts, Elaine E. Thompson, Michael E. Pique, Martin S. Perez, L. F. Ten Eyck</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-21T09:39:28.803263-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23304</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23304</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23304</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Computational docking is a useful tool for predicting macromolecular complexes, which are often difficult to determine experimentally. Here, we present the DOT2 software suite, an updated version of the DOT intermolecular docking program. DOT2 provides straightforward, automated construction of improved biophysical models based on molecular coordinates, offering checkpoints that guide the user to include critical features. DOT has been updated to run more quickly, allow flexibility in grid size and spacing, and generate an infinitive complete list of favorable candidate configurations. Output can be filtered by experimental data and rescored by the sum of electrostatic and atomic desolvation energies. We show that this rescoring method improves the ranking of correct complexes for a wide range of macromolecular interactions and demonstrate that biologically relevant models are essential for biologically relevant results. The flexibility and versatility of DOT2 accommodate realistic models of complex biological systems, improving the likelihood of a successful docking outcome. © 2013 Wiley Periodicals, Inc.</p></div>
<a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/jcc.23304/asset/image_m/jcc23304-toc-0001-m.png?v=1&amp;s=0346a0cd6bc1fc436cee1f0545025f4f632b4b7b" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23304/asset/image_n/jcc23304-toc-0001.png?v=1&amp;s=638634a349f816b47a1c42cf08d34053a36459d5"/></a>
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Computational docking is a useful tool for predicting macromolecular complexes, which are often difficult to determine experimentally. Here, we present the DOT2 software suite, an updated version of the DOT intermolecular docking program. DOT2 provides straightforward, automated construction of improved biophysical models based on molecular coordinates, offering checkpoints that guide the user to include critical features. DOT has been updated to run more quickly, allow flexibility in grid size and spacing, and generate an infinitive complete list of favorable candidate configurations. Output can be filtered by experimental data and rescored by the sum of electrostatic and atomic desolvation energies. We show that this rescoring method improves the ranking of correct complexes for a wide range of macromolecular interactions and demonstrate that biologically relevant models are essential for biologically relevant results. The flexibility and versatility of DOT2 accommodate realistic models of complex biological systems, improving the likelihood of a successful docking outcome. © 2013 Wiley Periodicals, Inc.







</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23312" xmlns="http://purl.org/rss/1.0/"><title>Analytic derivatives for the XYG3 type of doubly hybrid density functionals: Theory, implementation, and assessment</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23312</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Analytic derivatives for the XYG3 type of doubly hybrid density functionals: Theory, implementation, and assessment</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Neil Qiang Su, Igor Ying Zhang, Xin Xu</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-16T22:10:32.032578-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23312</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23312</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23312</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>We present a theoretical development of the equations required to perform an analytic geometry optimization of a molecular system using the XYG3 type of doubly hybrid (xDH) functionals. In contrast to the well-established B2PLYP type of DH functionals, the energy expressions in the xDH functionals are constructed by using density and orbital information from another standard Kohn–Sham (KS) functional (e.g., B3LYP) for doing the self-consistent field calculations. Thus, the xDH functionals are nonvariational in both the hybrid density functional part and the second-order perturbation part, each of which requires formally to solve a coupled-perturbed KS equation. An implementation is reported here which combines the two parts by defining a total Lagrangian such that only a single set of the Z-vector equations need to be solved. The computational cost with our implementation is of the same order as those for the conventional Møller–Plesset theory to the second order (MP2) and B2PLYP. Systematic test calculations are provided for covalently bonded molecules as well as compounds involving the intramolecular nonbonded interactions for the main group elements. Satisfactory performance of the xDH functionals demonstrates that the extra computer time on top of the conventional KS procedure is well-invested, in particular, when the standard KS functionals and MP2 as well, are problematic. © 2013 Wiley Periodicals, Inc.</p></div>
<a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/jcc.23312/asset/image_m/jcc23312-toc-0001-m.png?v=1&amp;s=fbfba7e446b45db60a32ea2d3965c3befb1cad8c" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23312/asset/image_n/jcc23312-toc-0001.png?v=1&amp;s=3656c7f603f2f0236cb5c39831285312bcb7d7ca"/></a>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>The XYG3-type doubly hybrid (xDH) functionals are nonvariational in both the hybrid density functional part and the second-order perturbation part, each of which requires formally a coupled-perturbed Kohn–Sham equation to be solved for analytic gradients. An implementation is reported here which combines the two parts by defining a total Lagrangian such that only a single set of the Z-vector equations need to be solved. Test calculations are provided to demonstrate the satisfactory performance of the xDH functionals for geometry optimizations.
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We present a theoretical development of the equations required to perform an analytic geometry optimization of a molecular system using the XYG3 type of doubly hybrid (xDH) functionals. In contrast to the well-established B2PLYP type of DH functionals, the energy expressions in the xDH functionals are constructed by using density and orbital information from another standard Kohn–Sham (KS) functional (e.g., B3LYP) for doing the self-consistent field calculations. Thus, the xDH functionals are nonvariational in both the hybrid density functional part and the second-order perturbation part, each of which requires formally to solve a coupled-perturbed KS equation. An implementation is reported here which combines the two parts by defining a total Lagrangian such that only a single set of the Z-vector equations need to be solved. The computational cost with our implementation is of the same order as those for the conventional Møller–Plesset theory to the second order (MP2) and B2PLYP. Systematic test calculations are provided for covalently bonded molecules as well as compounds involving the intramolecular nonbonded interactions for the main group elements. Satisfactory performance of the xDH functionals demonstrates that the extra computer time on top of the conventional KS procedure is well-invested, in particular, when the standard KS functionals and MP2 as well, are problematic. © 2013 Wiley Periodicals, Inc.
The XYG3-type doubly hybrid (xDH) functionals are nonvariational in both the hybrid density functional part and the second-order perturbation part, each of which requires formally a coupled-perturbed Kohn–Sham equation to be solved for analytic gradients. An implementation is reported here which combines the two parts by defining a total Lagrangian such that only a single set of the Z-vector equations need to be solved. Test calculations are provided to demonstrate the satisfactory performance of the xDH functionals for geometry optimizations.






</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23303" xmlns="http://purl.org/rss/1.0/"><title>Nonfitting protein–ligand interaction scoring function based on first-principles theoretical chemistry methods: Development and application on kinase inhibitors</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23303</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Nonfitting protein–ligand interaction scoring function based on first-principles theoretical chemistry methods: Development and application on kinase inhibitors</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Li Rao, Igor Ying Zhang, Wenping Guo, Li Feng, Eric Meggers, Xin Xu</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-16T08:33:04.763948-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23303</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23303</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23303</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Targeted therapy is currently a hot topic in the fields of cancer research and drug design. An important requirement for this approach is the development of potent and selective inhibitors for the identified target protein. However, current ways to estimate inhibitor efficacy rely on empirical protein–ligand interaction scoring functions which, suffering from their heavy parameterizations, often lead to a low accuracy. In this work, we develop a nonfitting scoring function, which consists of three terms: (1) gas-phase protein-ligand binding enthalpy obtained by the eXtended ONIOM hybrid method based on an integration of density functional theory (DFT) methods (XYG3 and ωB97X-D) and the semiempirical PM6 method, (2) solvation free energy based on DFT-SMD solvation model, and (3) entropy effect estimated by using DFT frequency analysis. The new scoring function is tested on a cyclin-dependent kinase 2 (CDK2) inhibitor database including 76 CDK2 protein inhibitors and a p21-activated kinase 1 (PAK1) inhibitor database including 20 organometallic PAK1 protein inhibitors. From the results, good correlations are found between the calculated scores and the experimental inhibitor efficacies with the square of correlation coefficient <em>R</em><sup>2</sup> of 0.76–0.88. This suggests a good predictive power of this scoring function. To the best of our knowledge, this is the first high level theory-based nonfitting scoring function with such a good level of performance. This scoring function is recommended to be used in the final screening of lead structure derivatives. © 2013 Wiley Periodicals, Inc.</p></div>
<a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/jcc.23303/asset/image_m/jcc23303-toc-0001-m.png?v=1&amp;s=c2a033421ea26dd2dc77577c6ae1c2c93ae797a2" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23303/asset/image_n/jcc23303-toc-0001.png?v=1&amp;s=e544af10bc9f56afde4ccdb3e0ed74ebf26668d1"/></a>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Accurate theoretical estimation of protein–ligand interaction is vitally important for the rational design of an effective drug. In this work, we have developed a nonfitting protein–ligand interaction scoring function based on divide and conquer strategy and first-principles methods. Good correlations on applications to cyclin-dependent kinase 2 and p21-activated kinase 1 inhibitor databases are found between the calculated scores and the experimental inhibitor efficacies with the square of correlation coefficient <em>R</em><sup>2</sup> of 0.76–0.89.
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Targeted therapy is currently a hot topic in the fields of cancer research and drug design. An important requirement for this approach is the development of potent and selective inhibitors for the identified target protein. However, current ways to estimate inhibitor efficacy rely on empirical protein–ligand interaction scoring functions which, suffering from their heavy parameterizations, often lead to a low accuracy. In this work, we develop a nonfitting scoring function, which consists of three terms: (1) gas-phase protein-ligand binding enthalpy obtained by the eXtended ONIOM hybrid method based on an integration of density functional theory (DFT) methods (XYG3 and ωB97X-D) and the semiempirical PM6 method, (2) solvation free energy based on DFT-SMD solvation model, and (3) entropy effect estimated by using DFT frequency analysis. The new scoring function is tested on a cyclin-dependent kinase 2 (CDK2) inhibitor database including 76 CDK2 protein inhibitors and a p21-activated kinase 1 (PAK1) inhibitor database including 20 organometallic PAK1 protein inhibitors. From the results, good correlations are found between the calculated scores and the experimental inhibitor efficacies with the square of correlation coefficient R2 of 0.76–0.88. This suggests a good predictive power of this scoring function. To the best of our knowledge, this is the first high level theory-based nonfitting scoring function with such a good level of performance. This scoring function is recommended to be used in the final screening of lead structure derivatives. © 2013 Wiley Periodicals, Inc.
Accurate theoretical estimation of protein–ligand interaction is vitally important for the rational design of an effective drug. In this work, we have developed a nonfitting protein–ligand interaction scoring function based on divide and conquer strategy and first-principles methods. Good correlations on applications to cyclin-dependent kinase 2 and p21-activated kinase 1 inhibitor databases are found between the calculated scores and the experimental inhibitor efficacies with the square of correlation coefficient R2 of 0.76–0.89.






</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23322" xmlns="http://purl.org/rss/1.0/"><title>Comment on “QSAR model reproducibility and applicability: A case study of rate constants of hydroxyl radical reaction models applied to polybrominated diphenyl ethers and (benzo-)triazoles”</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23322</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Comment on “QSAR model reproducibility and applicability: A case study of rate constants of hydroxyl radical reaction models applied to polybrominated diphenyl ethers and (benzo-)triazoles”</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Sierra Rayne</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-16T00:10:37.443971-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23322</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23322</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23322</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Letter to the Editor</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[]]></content:encoded><description/></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23324" xmlns="http://purl.org/rss/1.0/"><title>XPS of oxygen atoms on Ag(111) and Ag(110) surfaces: Accurate study with SAC/SAC-CI combined with dipped adcluster model</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23324</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">XPS of oxygen atoms on Ag(111) and Ag(110) surfaces: Accurate study with SAC/SAC-CI combined with dipped adcluster model</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Atsushi Ishikawa, Hiroshi Nakatsuji</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-16T00:10:33.867524-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23324</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23324</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23324</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>O1s core-electron binding energies (CEBE) of the atomic oxygens on different Ag surfaces were investigated by the symmetry adapted cluster-configuration interaction (SAC-CI) method combined with the dipped adcluster model, in which the electron exchange between bulk metal and adsorbate is taken into account properly. Electrophilic and nucleophilic oxygens (<em>O</em><sub>elec</sub> and <em>O</em><sub>nuc</sub>) that might be important for olefin epoxidation in a low-oxygen coverage condition were focused here. We consider the O1s CEBE as a key property to distinguish the surface oxygen states, and series of calculation was carried out by the Hartree–Fock, Density functional theory, and SAC/SAC-CI methods. The experimental information and our SAC/SAC-CI results indicate that <em>O</em><sub>elec</sub> is the atomic oxygen adsorbed on the fcc site of Ag(111) and that <em>O</em><sub>nuc</sub> is the one on the reconstructed added-row site of Ag(110) and that one- and two-electron transfers occur, respectively, to the <em>O</em><sub>elec</sub> and <em>O</em><sub>nuc</sub> adclusters from the silver surface. © 2013 Wiley Periodicals, Inc.</p></div>
<a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/jcc.23324/asset/image_m/jcc23324-toc-0001-m.png?v=1&amp;s=bf4e15708ad11c0668f52c5e8124b1c52964f7ad" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23324/asset/image_n/jcc23324-toc-0001.png?v=1&amp;s=ad2b4e01b88156e1b6220562ab58e13be8d84cc9"/></a>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>O1s core-electron binding energies of electrophilic and nucleophilic oxygens important for olefin epoxidation on silver surface were investigated by the symmetry-adapted-cluster configuration-interaction (SAC-CI) method combined with the dipped adcluster model (DAM). The experimental information and our theoretical results indicate that Oelec is the atomic oxygen adsorbed on the fcc site of Ag(111) and that Onuc is the one on the reconstructed added-row site of Ag(110).
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O1s core-electron binding energies (CEBE) of the atomic oxygens on different Ag surfaces were investigated by the symmetry adapted cluster-configuration interaction (SAC-CI) method combined with the dipped adcluster model, in which the electron exchange between bulk metal and adsorbate is taken into account properly. Electrophilic and nucleophilic oxygens (Oelec and Onuc) that might be important for olefin epoxidation in a low-oxygen coverage condition were focused here. We consider the O1s CEBE as a key property to distinguish the surface oxygen states, and series of calculation was carried out by the Hartree–Fock, Density functional theory, and SAC/SAC-CI methods. The experimental information and our SAC/SAC-CI results indicate that Oelec is the atomic oxygen adsorbed on the fcc site of Ag(111) and that Onuc is the one on the reconstructed added-row site of Ag(110) and that one- and two-electron transfers occur, respectively, to the Oelec and Onuc adclusters from the silver surface. © 2013 Wiley Periodicals, Inc.
O1s core-electron binding energies of electrophilic and nucleophilic oxygens important for olefin epoxidation on silver surface were investigated by the symmetry-adapted-cluster configuration-interaction (SAC-CI) method combined with the dipped adcluster model (DAM). The experimental information and our theoretical results indicate that Oelec is the atomic oxygen adsorbed on the fcc site of Ag(111) and that Onuc is the one on the reconstructed added-row site of Ag(110).






</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23316" xmlns="http://purl.org/rss/1.0/"><title>Performance of density functional theory in computing nonresonant vibrational (hyper)polarizabilities</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23316</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Performance of density functional theory in computing nonresonant vibrational (hyper)polarizabilities</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Ireneusz W. Bulik, Robert Zaleśny, Wojciech Bartkowiak, Josep M. Luis, Bernard Kirtman, Gustavo E. Scuseria, Aggelos Avramopoulos, Heribert Reis, Manthos G. Papadopoulos</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-16T00:10:29.126606-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23316</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23316</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23316</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">00</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">00</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A set of exchange-correlation functionals, including BLYP, PBE0, B3LYP, BHandHLYP, CAM-B3LYP, LC-BLYP, and HSE, has been used to determine static and dynamic nonresonant (nuclear relaxation) vibrational (hyper)polarizabilities for a series of all-<em>trans</em> polymethineimine (PMI) oligomers containing up to eight monomer units. These functionals are assessed against reference values obtained using the Møller–Plesset second-order perturbation theory (MP2) and CCSD methods. For the smallest oligomer, CCSD(T) calculations confirm the choice of MP2 and CCSD as appropriate for assessing the density functionals. By and large, CAM-B3LYP is the most successful, because it is best for the nuclear relaxation contribution to the static linear polarizability, intensity-dependent refractive index second hyperpolarizability, static second hyperpolarizability, and is close to the best for the electro-optical Pockels effect first hyperpolarizability. However, none of the functionals perform satisfactorily for all the vibrational (hyper)polarizabilities studied. In fact, in the case of electric field-induced second harmonic generation all of them, as well as the Hartree–Fock approximation, yield the wrong sign. We have also found that the Pople 6–31+G(d) basis set is unreliable for computing nuclear relaxation (hyper)polarizabilities of PMI oligomers due to the spurious prediction of a nonplanar equilibrium geometry. © 2013 Wiley Periodicals, Inc.</p></div>
<a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/jcc.23316/asset/image_m/jcc23316-toc-0001-m.png?v=1&amp;s=2a930289b082a7a17c1ef2c45a3d35af8bea1e2f" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23316/asset/image_n/jcc23316-toc-0001.png?v=1&amp;s=8d58fc0f68283671a7b4ef51871eb880857db8cd"/></a>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>A set of exchange-correlation functionals, including BLYP, PBE0, B3LYP, BHandHLYP, CAM-B3LYP, LC-BLYP, and HSE, has been used to determine static and dynamic nonresonant (nuclear relaxation) vibrational (hyper)polarizabilities for a series of polymethineimine oligomers containing up to eight monomer units. These functionals are assessed against reference values obtained using the MP2 and CCSD methods.
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A set of exchange-correlation functionals, including BLYP, PBE0, B3LYP, BHandHLYP, CAM-B3LYP, LC-BLYP, and HSE, has been used to determine static and dynamic nonresonant (nuclear relaxation) vibrational (hyper)polarizabilities for a series of all-trans polymethineimine (PMI) oligomers containing up to eight monomer units. These functionals are assessed against reference values obtained using the Møller–Plesset second-order perturbation theory (MP2) and CCSD methods. For the smallest oligomer, CCSD(T) calculations confirm the choice of MP2 and CCSD as appropriate for assessing the density functionals. By and large, CAM-B3LYP is the most successful, because it is best for the nuclear relaxation contribution to the static linear polarizability, intensity-dependent refractive index second hyperpolarizability, static second hyperpolarizability, and is close to the best for the electro-optical Pockels effect first hyperpolarizability. However, none of the functionals perform satisfactorily for all the vibrational (hyper)polarizabilities studied. In fact, in the case of electric field-induced second harmonic generation all of them, as well as the Hartree–Fock approximation, yield the wrong sign. We have also found that the Pople 6–31+G(d) basis set is unreliable for computing nuclear relaxation (hyper)polarizabilities of PMI oligomers due to the spurious prediction of a nonplanar equilibrium geometry. © 2013 Wiley Periodicals, Inc.
A set of exchange-correlation functionals, including BLYP, PBE0, B3LYP, BHandHLYP, CAM-B3LYP, LC-BLYP, and HSE, has been used to determine static and dynamic nonresonant (nuclear relaxation) vibrational (hyper)polarizabilities for a series of polymethineimine oligomers containing up to eight monomer units. These functionals are assessed against reference values obtained using the MP2 and CCSD methods.






</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23317" xmlns="http://purl.org/rss/1.0/"><title>Corrected small basis set Hartree-Fock method for large systems</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23317</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Corrected small basis set Hartree-Fock method for large systems</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Rebecca Sure, Stefan Grimme</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-14T00:26:22.229904-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23317</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23317</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23317</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">00</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">00</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A quantum chemical method based on a Hartree-Fock calculation with a small Gaussian AO basis set is presented. Its main area of application is the computation of structures, vibrational frequencies, and noncovalent interaction energies in huge molecular systems. The method is suggested as a partial replacement of semiempirical approaches or density functional theory (DFT) in particular when self-interaction errors are acute. In order to get accurate results three physically plausible atom pair-wise correction terms are applied for London dispersion interactions (D3 scheme), basis set superposition error (gCP scheme), and short-ranged basis set incompleteness effects. In total nine global empirical parameters are used. This so-called Hartee-Fock-3c (HF-3c) method is tested for geometries of small organic molecules, interaction energies and geometries of noncovalently bound complexes, for supramolecular systems, and protein structures. In the majority of realistic test cases good results approaching large basis set DFT quality are obtained at a tiny fraction of computational cost. © 2013 Wiley Periodicals, Inc.</p></div>
<a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/jcc.23317/asset/image_m/jcc23317-toc-0001-m.png?v=1&amp;s=af39bc1f2cf78b40aaaf23732f160c8b515b0550" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23317/asset/image_n/jcc23317-toc-0001.png?v=1&amp;s=ece4a230021b26e84f917adfe82cede6dc8c9b24"/></a>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>A newly developed HF-3c quantum chemical protocol combines a Hartree- Fock/small basis set calculation with  three physically plausible atom-pair wise correction terms. It yields good results for non-covalent  interactions, geometries of organic molecules, supramolecular complexes and small proteins.    For most test cases its accuracy approaches DFT-D3/large basis set quality, but obtained at a tiny  fraction of computational cost and can  hence be applied to large molecular systems as an alternative to semiempirical methods. 
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A quantum chemical method based on a Hartree-Fock calculation with a small Gaussian AO basis set is presented. Its main area of application is the computation of structures, vibrational frequencies, and noncovalent interaction energies in huge molecular systems. The method is suggested as a partial replacement of semiempirical approaches or density functional theory (DFT) in particular when self-interaction errors are acute. In order to get accurate results three physically plausible atom pair-wise correction terms are applied for London dispersion interactions (D3 scheme), basis set superposition error (gCP scheme), and short-ranged basis set incompleteness effects. In total nine global empirical parameters are used. This so-called Hartee-Fock-3c (HF-3c) method is tested for geometries of small organic molecules, interaction energies and geometries of noncovalently bound complexes, for supramolecular systems, and protein structures. In the majority of realistic test cases good results approaching large basis set DFT quality are obtained at a tiny fraction of computational cost. © 2013 Wiley Periodicals, Inc.
A newly developed HF-3c quantum chemical protocol combines a Hartree- Fock/small basis set calculation with  three physically plausible atom-pair wise correction terms. It yields good results for non-covalent  interactions, geometries of organic molecules, supramolecular complexes and small proteins.    For most test cases its accuracy approaches DFT-D3/large basis set quality, but obtained at a tiny  fraction of computational cost and can  hence be applied to large molecular systems as an alternative to semiempirical methods. 






</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23311" xmlns="http://purl.org/rss/1.0/"><title>Cytochrome P450 compound I in the plane-wave pseudopotential framework: GGA electronic and geometric structure of thiolate-ligated iron(IV)–oxo porphyrin</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23311</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Cytochrome P450 compound I in the plane-wave pseudopotential framework: GGA electronic and geometric structure of thiolate-ligated iron(IV)–oxo porphyrin</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Justin E. Elenewski, John C Hackett</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-14T00:18:27.316937-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23311</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23311</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23311</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The cytochromes P450 constitute a ubiquitous family of metalloenzymes, catalyzing manifold reactions of biological and synthetic importance via a thiolate-ligated iron-oxo (IV) porphyrin radical species denoted compound I (Cpd I). Experimental investigations have implicated this intermediate in a broad spectrum of biophysically interesting phenomena, further augmenting the importance of a Cpd I model system. <em>Ab initio</em> molecular dynamics, including Car–Parrinello and path integral methods, conjoin electronic structure theory with finite temperature simulation, affording tools most valuable to approach such enzymes. These methods are typically driven by density functional theory (DFT) in a plane-wave pseudopotential framework; however, existing studies of Cpd I have been restricted to localized Gaussian basis sets. The appropriate choice of density functional and pseudopotential for such simulations is accordingly not obvious. To remedy this situation, a systematic benchmarking of thiolate-ligated Cpd I is performed using several generalized-gradient approximation (GGA) functionals in the Martins–Troullier and Vanderbilt ultrasoft pseudopotential schemes. The resultant electronic and structural parameters are compared to localized–basis DFT calculations using GGA and hybrid density functionals. The merits and demerits of each scheme are presented in the context of reproducing existing experimental and theoretical results for Cpd I. © 2013 Wiley Periodicals, Inc.</p></div>
<a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/jcc.23311/asset/image_m/jcc23311-toc-0001-m.png?v=1&amp;s=a97182bf741124441415b7f1490ac810dfe7d0ac" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23311/asset/image_n/jcc23311-toc-0001.png?v=1&amp;s=5bebb37984a924f79131585417d910f29cc058ae"/></a>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>The thiolate-ligated iron(IV)-oxo porphyrins, known as collectively as thiolate compound I, are potent and ubiquitous oxidizing agents active in both the cytochrome P450 superfamily of enzymes and in several highly reactive synthetic complexes. This particular species is characterized for the first time in a plane-wave density functional theory framework and benchmarked with respect to established localized-basis calculations.
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The cytochromes P450 constitute a ubiquitous family of metalloenzymes, catalyzing manifold reactions of biological and synthetic importance via a thiolate-ligated iron-oxo (IV) porphyrin radical species denoted compound I (Cpd I). Experimental investigations have implicated this intermediate in a broad spectrum of biophysically interesting phenomena, further augmenting the importance of a Cpd I model system. Ab initio molecular dynamics, including Car–Parrinello and path integral methods, conjoin electronic structure theory with finite temperature simulation, affording tools most valuable to approach such enzymes. These methods are typically driven by density functional theory (DFT) in a plane-wave pseudopotential framework; however, existing studies of Cpd I have been restricted to localized Gaussian basis sets. The appropriate choice of density functional and pseudopotential for such simulations is accordingly not obvious. To remedy this situation, a systematic benchmarking of thiolate-ligated Cpd I is performed using several generalized-gradient approximation (GGA) functionals in the Martins–Troullier and Vanderbilt ultrasoft pseudopotential schemes. The resultant electronic and structural parameters are compared to localized–basis DFT calculations using GGA and hybrid density functionals. The merits and demerits of each scheme are presented in the context of reproducing existing experimental and theoretical results for Cpd I. © 2013 Wiley Periodicals, Inc.
The thiolate-ligated iron(IV)-oxo porphyrins, known as collectively as thiolate compound I, are potent and ubiquitous oxidizing agents active in both the cytochrome P450 superfamily of enzymes and in several highly reactive synthetic complexes. This particular species is characterized for the first time in a plane-wave density functional theory framework and benchmarked with respect to established localized-basis calculations.






</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23309" xmlns="http://purl.org/rss/1.0/"><title>Quantum wave-packet and quasiclassical trajectory studies of the reaction H(2S) + CH(X2Π; v = 0, j = 1) → C(1D) + H2(X1
Σg+): Coriolis coupling effects and stereodynamics</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23309</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Quantum wave-packet and quasiclassical trajectory studies of the reaction H(2S) + CH(X2Π; v = 0, j = 1) → C(1D) + H2(X1
Σg+): Coriolis coupling effects and stereodynamics</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Ruifeng Lu, Yunhui Wang, Kaiming Deng</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-14T00:04:50.519034-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23309</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23309</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23309</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The quantum mechanics (QM) and quasiclassical trajectory (QCT) calculations have been carried out for the title reaction with the ground minimal allowed rotational state of CH (<em>j</em> = 1) on the 1 <sup>1</sup>A′ potential energy surface. For the reaction probability at total angular momentum <em>J</em> = 0, a similar trend of the QM and QCT calculations is observed, and the QM results are larger than the latter almost in the whole considered energy range (0.1–1.5 eV). The QCT integral cross sections are larger than the QM results with centrifugal sudden approximation, while smaller than those from QM method including Coriolis coupling for collision energies bigger than 0.25 eV. The quantum wave-packet computations show that the Coriolis coupling effects get more and more pronounced with increasing of <em>J</em>. In addition to the scalar properties, the stereodynamical properties, such as the average rotational alignment factor &lt;<em>P</em><sub>2</sub>(<b><em>j</em>′•<em>k</em></b>)&gt;, the angular distributions <em>P</em>(θ<sub>r</sub>), <em>P</em>(ϕ<sub>r</sub>), <em>P</em>(θ<sub>r</sub>,ϕ<sub>r</sub>), and the polarization-dependent generalized differential cross sections have been explored in detail by QCT approach. © 2013 Wiley Periodicals, Inc.</p></div>
<a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/jcc.23309/asset/image_m/jcc23309-toc-0001-m.png?v=1&amp;s=5776bfc7e529b65a0ac82efc12c0bec5754d8124" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23309/asset/image_n/jcc23309-toc-0001.png?v=1&amp;s=cb0619441772b9ae0093641d730fae5e8b44e959"/></a>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>The CH<sub>2</sub> system plays an important role in atmospheric and combustion chemistry, thus, to know clearly the chemically dynamical properties will be of great importance. For H(<sup>2</sup>S) + CH(X<sup>2</sup>Π) → C(<sup>1</sup>D) + H<sub>2</sub>(X<sup>1</sup>
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23309/asset/equation/jcc23309-math-0009.gif?v=1&amp;t=hh0hhazq&amp;s=c5e2a67c2be9ee2ebada1410967cdd58fcb0da1d" class="inlineGraphic"/>), we presented the full information of reaction probability, integral cross section and rate constants, various angular distributions as well as the extracted polarization-dependent differential cross-sections. Both quasiclassical trajectory and time-dependent quantum wave-packet methods were carried out on BHL PES.
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The quantum mechanics (QM) and quasiclassical trajectory (QCT) calculations have been carried out for the title reaction with the ground minimal allowed rotational state of CH (j = 1) on the 1 1A′ potential energy surface. For the reaction probability at total angular momentum J = 0, a similar trend of the QM and QCT calculations is observed, and the QM results are larger than the latter almost in the whole considered energy range (0.1–1.5 eV). The QCT integral cross sections are larger than the QM results with centrifugal sudden approximation, while smaller than those from QM method including Coriolis coupling for collision energies bigger than 0.25 eV. The quantum wave-packet computations show that the Coriolis coupling effects get more and more pronounced with increasing of J. In addition to the scalar properties, the stereodynamical properties, such as the average rotational alignment factor &lt;P2(j′•k)&gt;, the angular distributions P(θr), P(ϕr), P(θr,ϕr), and the polarization-dependent generalized differential cross sections have been explored in detail by QCT approach. © 2013 Wiley Periodicals, Inc.
The CH2 system plays an important role in atmospheric and combustion chemistry, thus, to know clearly the chemically dynamical properties will be of great importance. For H(2S) + CH(X2Π) → C(1D) + H2(X1
Σg+), we presented the full information of reaction probability, integral cross section and rate constants, various angular distributions as well as the extracted polarization-dependent differential cross-sections. Both quasiclassical trajectory and time-dependent quantum wave-packet methods were carried out on BHL PES.






</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23305" xmlns="http://purl.org/rss/1.0/"><title>A simple but effective modeling strategy for structural properties of non-heme Fe(II) sites in proteins: Test of force field models and application to proteins in the AlkB family</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23305</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">A simple but effective modeling strategy for structural properties of non-heme Fe(II) sites in proteins: Test of force field models and application to proteins in the AlkB family</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Xueqin Pang, Keli Han, Qiang Cui</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-13T01:06:10.447068-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23305</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23305</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23305</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>To facilitate computational study of proteins in the AlkB family and related α-ketoglutarate/Fe(II)-dependent dioxygenases, we have tested a simple modeling strategy for the non-heme Fe(II) site in which the iron is represented by a simple +2 point charge with Lennard-Jones parameters. Calculations for an AlkB active site model in the gas phase and ∼150 ns molecular dynamics (MD) simulations for two enzyme-dsDNA complexes (<em>E. coli</em> AlkB-dsDNA and ABH2-dsDNA) suggest that this simple modeling strategy provides a satisfactory description of structural properties of the Fe(II) site in AlkB enzymes, provided that care is exercised to control the binding mode of carboxylate (Asp) to the iron. MD simulations using the model for AlkB-dsDNA and ABH2-dsDNA systems find that although the structural features for the latter are overall in good agreement with the crystal structure, the dsDNA, and AlkB-dsDNA interface undergo substantial changes during the MD simulations from the crystal structure. Even for ABH2, new interactions form between a long loop region and dsDNA upon structural relaxation of the loop, supporting the role of this loop in DNA binding despite the lack of interactions between them in the crystal structure. Analysis of DNA backbone torsional distributions helps identify regions that adopt strained conformations. Collectively, the results highlight that crystal packing may have a significant impact on the structure of protein-DNA complexes; the simulations also provide additional insights regarding why AlkB and ABH2 prefer single-strand and double-strand DNA, respectively, as substrate. © 2013 Wiley Periodicals, Inc.</p></div>
<a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/jcc.23305/asset/image_m/jcc23305-toc-0001-m.png?v=1&amp;s=85864aca7753487292c8c6ea46ece64ce7d5989a" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23305/asset/image_n/jcc23305-toc-0001.png?v=1&amp;s=4ab2d8e47588135699577a25c275137f84cc9b19"/></a>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>A simple molecular mechanics model for the non-heme Fe(II) site is developed and tested using molecular dynamics simulations for enzymes in the AlkB family. Although structural features for the ABH2-dsDNA complex are overall in good agreement with the crystal structure, the dsDNA and AlkB-dsDNA interface undergo substantial changes. The results highlight that crystal packing may have a significant impact on the structure of protein-DNA complexes and provide additional insights regarding substrate specificity of AlkB enzymes.
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To facilitate computational study of proteins in the AlkB family and related α-ketoglutarate/Fe(II)-dependent dioxygenases, we have tested a simple modeling strategy for the non-heme Fe(II) site in which the iron is represented by a simple +2 point charge with Lennard-Jones parameters. Calculations for an AlkB active site model in the gas phase and ∼150 ns molecular dynamics (MD) simulations for two enzyme-dsDNA complexes (E. coli AlkB-dsDNA and ABH2-dsDNA) suggest that this simple modeling strategy provides a satisfactory description of structural properties of the Fe(II) site in AlkB enzymes, provided that care is exercised to control the binding mode of carboxylate (Asp) to the iron. MD simulations using the model for AlkB-dsDNA and ABH2-dsDNA systems find that although the structural features for the latter are overall in good agreement with the crystal structure, the dsDNA, and AlkB-dsDNA interface undergo substantial changes during the MD simulations from the crystal structure. Even for ABH2, new interactions form between a long loop region and dsDNA upon structural relaxation of the loop, supporting the role of this loop in DNA binding despite the lack of interactions between them in the crystal structure. Analysis of DNA backbone torsional distributions helps identify regions that adopt strained conformations. Collectively, the results highlight that crystal packing may have a significant impact on the structure of protein-DNA complexes; the simulations also provide additional insights regarding why AlkB and ABH2 prefer single-strand and double-strand DNA, respectively, as substrate. © 2013 Wiley Periodicals, Inc.
A simple molecular mechanics model for the non-heme Fe(II) site is developed and tested using molecular dynamics simulations for enzymes in the AlkB family. Although structural features for the ABH2-dsDNA complex are overall in good agreement with the crystal structure, the dsDNA and AlkB-dsDNA interface undergo substantial changes. The results highlight that crystal packing may have a significant impact on the structure of protein-DNA complexes and provide additional insights regarding substrate specificity of AlkB enzymes.






</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23315" xmlns="http://purl.org/rss/1.0/"><title>Multiobjective evolutionary algorithm with many tables for purely ab initio protein structure prediction</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23315</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Multiobjective evolutionary algorithm with many tables for purely ab initio protein structure prediction</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Christiane Regina Soares Brasil, Alexandre Claudio Botazzo Delbem, Fernando Luís Barroso da Silva</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-11T01:12:03.4057-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23315</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23315</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23315</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>This article focuses on the development of an approach for <em>ab initio</em> protein structure prediction (PSP) without using any earlier knowledge from similar protein structures, as fragment-based statistics or inference of secondary structures. Such an approach is called purely <em>ab initio</em> prediction. The article shows that well-designed multiobjective evolutionary algorithms can predict relevant protein structures in a purely <em>ab initio</em> way. One challenge for purely <em>ab initio</em> PSP is the prediction of structures with β-sheets. To work with such proteins, this research has also developed procedures to efficiently estimate hydrogen bond and solvation contribution energies. Considering van der Waals, electrostatic, hydrogen bond, and solvation contribution energies, the PSP is a problem with four energetic terms to be minimized. Each interaction energy term can be considered an objective of an optimization method. Combinatorial problems with four objectives have been considered too complex for the available multiobjective optimization (MOO) methods. The proposed approach, called “Multiobjective evolutionary algorithms with many tables” (MEAMT), can efficiently deal with four objectives through the combination thereof, performing a more adequate sampling of the objective space. Therefore, this method can better map the promising regions in this space, predicting structures in a purely <em>ab initio</em> way. In other words, MEAMT is an efficient optimization method for MOO, which explores simultaneously the search space as well as the objective space. MEAMT can predict structures with one or two domains with RMSDs comparable to values obtained by recently developed <em>ab initio</em> methods (GAPF<em><sub>CG</sub></em>, I-PAES, and Quark) that use different levels of earlier knowledge. © 2013 Wiley Periodicals, Inc.</p></div>
<a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/jcc.23315/asset/image_m/jcc23315-toc-0001-m.png?v=1&amp;s=29d37529521ac9ccbef661e531cf420ba5ba5682" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23315/asset/image_n/jcc23315-toc-0001.png?v=1&amp;s=686bafdc35046c42edad6cc4dfe7a4127d95266b"/></a>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Presenting computational optimization methods that can predict protein secondary structures—α-helix and β-sheet—without any earlier knowledge, mimicking what occurs in nature, that is, using only interaction energy terms involved in the formation of protein structures. The proposed approach, called Multiobjective evolutionary algorithms with many tables (MEAMT), can perform a more adequate sampling of the objective space. MEAMT is an efficient optimization method for multiobjective optimization, which explores simultaneously the search space as well as the objective space.
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This article focuses on the development of an approach for ab initio protein structure prediction (PSP) without using any earlier knowledge from similar protein structures, as fragment-based statistics or inference of secondary structures. Such an approach is called purely ab initio prediction. The article shows that well-designed multiobjective evolutionary algorithms can predict relevant protein structures in a purely ab initio way. One challenge for purely ab initio PSP is the prediction of structures with β-sheets. To work with such proteins, this research has also developed procedures to efficiently estimate hydrogen bond and solvation contribution energies. Considering van der Waals, electrostatic, hydrogen bond, and solvation contribution energies, the PSP is a problem with four energetic terms to be minimized. Each interaction energy term can be considered an objective of an optimization method. Combinatorial problems with four objectives have been considered too complex for the available multiobjective optimization (MOO) methods. The proposed approach, called “Multiobjective evolutionary algorithms with many tables” (MEAMT), can efficiently deal with four objectives through the combination thereof, performing a more adequate sampling of the objective space. Therefore, this method can better map the promising regions in this space, predicting structures in a purely ab initio way. In other words, MEAMT is an efficient optimization method for MOO, which explores simultaneously the search space as well as the objective space. MEAMT can predict structures with one or two domains with RMSDs comparable to values obtained by recently developed ab initio methods (GAPFCG, I-PAES, and Quark) that use different levels of earlier knowledge. © 2013 Wiley Periodicals, Inc.
Presenting computational optimization methods that can predict protein secondary structures—α-helix and β-sheet—without any earlier knowledge, mimicking what occurs in nature, that is, using only interaction energy terms involved in the formation of protein structures. The proposed approach, called Multiobjective evolutionary algorithms with many tables (MEAMT), can perform a more adequate sampling of the objective space. MEAMT is an efficient optimization method for multiobjective optimization, which explores simultaneously the search space as well as the objective space.






</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23310" xmlns="http://purl.org/rss/1.0/"><title>Accurate double many-body expansion potential energy surface by extrapolation to the complete basis set limit and dynamics calculations for ground state of NH2</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23310</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Accurate double many-body expansion potential energy surface by extrapolation to the complete basis set limit and dynamics calculations for ground state of NH2</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Yongqing Li, Jiuchuang Yuan, Maodu Chen, Fengcai Ma, Mengtao Sun</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-10T08:56:41.84042-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23310</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23310</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23310</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>An accurate single-sheeted double many-body expansion potential energy surface is reported for the title system. A switching function formalism has been used to warrant the correct behavior at the 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23310/asset/equation/jcc23310-math-0001.gif?v=1&amp;t=hh0hhb17&amp;s=abeb931769b8be368ba132b4328287d53817657b" class="inlineGraphic"/> and 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23310/asset/equation/jcc23310-math-0002.gif?v=1&amp;t=hh0hhb18&amp;s=fe59292dd1deaf5c297a298f6516aa233b5fe541" class="inlineGraphic"/> dissociation channels involving nitrogen in the ground 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23310/asset/equation/jcc23310-math-0003.gif?v=1&amp;t=hh0hhb18&amp;s=fe591856d554116a4c3abc55deeb8bb7f7627a80" class="inlineGraphic"/> and first excited 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23310/asset/equation/jcc23310-math-0004.gif?v=1&amp;t=hh0hhb19&amp;s=bee5b24965aef6729626a299527a730f6b37dcd2" class="inlineGraphic"/> states. The topographical features of the novel global potential energy surface are examined in detail, and found to be in good agreement with those calculated directly from the raw <em>ab initio</em> energies, as well as previous calculations available in the literature. The novel surface can be using to treat well the Renner–Teller degeneracy of the 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23310/asset/equation/jcc23310-math-0005.gif?v=1&amp;t=hh0hhb1a&amp;s=e0628b707dbee5b53689b46891d9823963a043e7" class="inlineGraphic"/> and 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23310/asset/equation/jcc23310-math-0006.gif?v=1&amp;t=hh0hhb1b&amp;s=2829748fdf24c3a8709c6557e8aecf8ad6078aed" class="inlineGraphic"/> states of 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23310/asset/equation/jcc23310-math-0007.gif?v=1&amp;t=hh0hhb1b&amp;s=128463ac8e16408bf2bdbcfeccca85a2f2008ad9" class="inlineGraphic"/>. Such a work can both be recommended for dynamics studies of the 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23310/asset/equation/jcc23310-math-0008.gif?v=1&amp;t=hh0hhb1b&amp;s=467aeda5f80f639338e65ad645d8f4d9a8fea610" class="inlineGraphic"/> reaction and as building blocks for constructing the double many-body expansion potential energy surface of larger nitrogen/hydrogen-containing systems. In turn, a test theoretical study of the reaction 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23310/asset/equation/jcc23310-math-0009.gif?v=1&amp;t=hh0hhb1d&amp;s=ab1ec72a9f4741fa0aab90f736c3bd4739ee0b32" class="inlineGraphic"/> has been carried out with the method of quantum wave packet on the new potential energy surface. Reaction probabilities, integral cross sections, and differential cross sections have been calculated. Threshold exists because of the energy barrier (68.5 meV) along the minimum energy path. On the curve of reaction probability for total angular momentum <em>J</em> = 0, there are two sharp peaks just above threshold. The value of integral cross section increases quickly from zero to maximum with the increase of collision energy, and then stays stable with small oscillations. The differential cross section result shows that the reaction is a typical forward and backward scatter in agreement with experimental measurement result. © 2013 Wiley Periodicals, Inc.</p></div>
<a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/jcc.23310/asset/image_m/jcc23310-toc-0001-m.png?v=1&amp;s=20f52012dbdff9c2509499504585479291359c62" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23310/asset/image_n/jcc23310-toc-0001.png?v=1&amp;s=c256bb62fe64302136acd962ae84900c71a278e8"/></a>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>A novel accurate potential energy surface and quantum wave packet dynamics calculations are reported for ground state of 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23310/asset/equation/jcc23310-math-0010.gif?v=1&amp;t=hh0hhb1h&amp;s=fed81274a57359c094eaa751688d82d7cf5b42de" class="inlineGraphic"/>. The novel potential energy surface can both be recommended for dynamics studies of the 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23310/asset/equation/jcc23310-math-0011.gif?v=1&amp;t=hh0hhb1i&amp;s=d7331e527228598da62ad6a1ffc7ed02f3f4e632" class="inlineGraphic"/> reaction and as building blocks for constructing the DMBE/CBS potential energy surface of larger nitrogen/hydrogen-containing systems. In particular, this new surface can be using for studding the Renner–Teller degeneracy of the 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23310/asset/equation/jcc23310-math-0012.gif?v=1&amp;t=hh0hhb1j&amp;s=0b57396d17c74f839408870f1b44ff68bfd5d3ed" class="inlineGraphic"/> and 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23310/asset/equation/jcc23310-math-0013.gif?v=1&amp;t=hh0hhb1j&amp;s=a151fbadee65b754293169b4ef508fa1267f7cac" class="inlineGraphic"/> states of 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23310/asset/equation/jcc23310-math-0014.gif?v=1&amp;t=hh0hhb1k&amp;s=2ec41acf802ad486195835a030333fd031a1740e" class="inlineGraphic"/>.
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An accurate single-sheeted double many-body expansion potential energy surface is reported for the title system. A switching function formalism has been used to warrant the correct behavior at the 
H2(X1Σg+)+N(2D) and 
NH (X3Σ−)+H(2S) dissociation channels involving nitrogen in the ground 
N(4S) and first excited 
N(2D) states. The topographical features of the novel global potential energy surface are examined in detail, and found to be in good agreement with those calculated directly from the raw ab initio energies, as well as previous calculations available in the literature. The novel surface can be using to treat well the Renner–Teller degeneracy of the 
12A″ and 
12A′ states of 
NH 2. Such a work can both be recommended for dynamics studies of the 
N(2D)+H2 reaction and as building blocks for constructing the double many-body expansion potential energy surface of larger nitrogen/hydrogen-containing systems. In turn, a test theoretical study of the reaction 
N(2D)+H2(X1Σg+)(ν=0,j=0)→NH (X3Σ−)+H(2S) has been carried out with the method of quantum wave packet on the new potential energy surface. Reaction probabilities, integral cross sections, and differential cross sections have been calculated. Threshold exists because of the energy barrier (68.5 meV) along the minimum energy path. On the curve of reaction probability for total angular momentum J = 0, there are two sharp peaks just above threshold. The value of integral cross section increases quickly from zero to maximum with the increase of collision energy, and then stays stable with small oscillations. The differential cross section result shows that the reaction is a typical forward and backward scatter in agreement with experimental measurement result. © 2013 Wiley Periodicals, Inc.
A novel accurate potential energy surface and quantum wave packet dynamics calculations are reported for ground state of 
NH 2. The novel potential energy surface can both be recommended for dynamics studies of the 
N(2D)+H2 reaction and as building blocks for constructing the DMBE/CBS potential energy surface of larger nitrogen/hydrogen-containing systems. In particular, this new surface can be using for studding the Renner–Teller degeneracy of the 
12A′ and 
12A″ states of 
NH 2.






</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23308" xmlns="http://purl.org/rss/1.0/"><title>Fast and accurate generation of ab initio quality atomic charges using nonparametric statistical regression</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23308</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Fast and accurate generation of ab initio quality atomic charges using nonparametric statistical regression</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Brajesh K. Rai, Gregory A. Bakken</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-07T09:28:19.824862-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23308</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23308</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23308</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>We introduce a class of partial atomic charge assignment method that provides <em>ab initio</em> quality description of the electrostatics of bioorganic molecules. The method uses a set of models that neither have a fixed functional form nor require a fixed set of parameters, and therefore are capable of capturing the complexities of the charge distribution in great detail. Random Forest regression is used to build separate charge models for elements H, C, N, O, F, S, and Cl, using training data consisting of partial charges along with a description of their surrounding chemical environments; training set charges are generated by fitting to the b3lyp/6-31G* electrostatic potential (ESP) and are subsequently <em>refined</em> to improve consistency and transferability of the charge assignments. Using a set of 210 neutral, small organic molecules, the absolute hydration free energy calculated using these charges in conjunction with Generalized Born solvation model shows a low mean unsigned error, close to 1 kcal/mol, from the experimental data. Using another large and independent test set of chemically diverse organic molecules, the method is shown to accurately reproduce charge-dependent observables—ESP and dipole moment—from <em>ab initio</em> calculations. The method presented here automatically provides an estimate of potential errors in the charge assignment, enabling systematic improvement of these models using additional data. This work has implications not only for the future development of charge models but also in developing methods to describe many other chemical properties that require accurate representation of the electronic structure of the system. © 2013 Wiley Periodicals, Inc.</p></div>
<a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/jcc.23308/asset/image_m/jcc23308-toc-0001-m.png?v=1&amp;s=60e24cca75e06d6fc20541ebe273923d7ccef293" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23308/asset/image_n/jcc23308-toc-0001.png?v=1&amp;s=fff50e745736a8e1e29a03e39ad8b2a6e40a90bd"/></a>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>We introduce a class of partial atomic charge assignment method that provides <em>ab initio</em> quality description of the electrostatics of bioorganic molecules. The method uses a set of models that neither have a fixed functional form nor require a fixed set of parameters, and therefore are capable of capturing the complexities of the charge distribution in great detail.
</p><!--Unmatched element: w:blockFixed--></div>
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We introduce a class of partial atomic charge assignment method that provides ab initio quality description of the electrostatics of bioorganic molecules. The method uses a set of models that neither have a fixed functional form nor require a fixed set of parameters, and therefore are capable of capturing the complexities of the charge distribution in great detail. Random Forest regression is used to build separate charge models for elements H, C, N, O, F, S, and Cl, using training data consisting of partial charges along with a description of their surrounding chemical environments; training set charges are generated by fitting to the b3lyp/6-31G* electrostatic potential (ESP) and are subsequently refined to improve consistency and transferability of the charge assignments. Using a set of 210 neutral, small organic molecules, the absolute hydration free energy calculated using these charges in conjunction with Generalized Born solvation model shows a low mean unsigned error, close to 1 kcal/mol, from the experimental data. Using another large and independent test set of chemically diverse organic molecules, the method is shown to accurately reproduce charge-dependent observables—ESP and dipole moment—from ab initio calculations. The method presented here automatically provides an estimate of potential errors in the charge assignment, enabling systematic improvement of these models using additional data. This work has implications not only for the future development of charge models but also in developing methods to describe many other chemical properties that require accurate representation of the electronic structure of the system. © 2013 Wiley Periodicals, Inc.
We introduce a class of partial atomic charge assignment method that provides ab initio quality description of the electrostatics of bioorganic molecules. The method uses a set of models that neither have a fixed functional form nor require a fixed set of parameters, and therefore are capable of capturing the complexities of the charge distribution in great detail.






</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23307" xmlns="http://purl.org/rss/1.0/"><title>PathOpt—A global transition state search approach: Outline of algorithm</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23307</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">PathOpt—A global transition state search approach: Outline of algorithm</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Christoph Grebner, Lukas P. Pason, Bernd Engels</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-04T11:33:50.513831-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23307</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23307</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23307</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">000</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">000</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>We propose a new algorithm to determine reaction paths and test its capability for Ar<sub>12</sub> and Ar<sub>13</sub> clusters. Its main ingredient is a search for the local minima on a (<em>n</em>−1) dimensional hyperplane (<em>n</em> = dimension of the complete system in Cartesian coordinates) lying perpendicular to the straight line connection between initial and final states. These minima are part of possible reaction paths and are, hence, used as starting points for an uphill search to the next transition state. First, path fragments are obtained from subsequent relaxations starting from these transition states. They can be combined with information from the straight line connection procedure to obtain complete paths. Our test computations for Ar<sub>12</sub> and Ar<sub>13</sub> clusters prove that PathOpt delivers several reaction paths in one round. © 2013 Wiley Periodicals, Inc.</p></div>
<a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/jcc.23307/asset/image_m/jcc23307-toc-0001-m.png?v=1&amp;s=b9d719ea0c388de1144b2c09c704cb0c11c7ea02" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23307/asset/image_n/jcc23307-toc-0001.png?v=1&amp;s=02c9e457346223ccb2f2c521d650af451303e699"/></a>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Knowledge about possible transition and reaction pathways is of utmost importance for the description of many processes like protein folding or complex enzymatic reactions. We propose a new algorithm based on a global optimization in a reduced phase space to locate possible transition states between reactants and products. Investigations for Ar<sub>12</sub> and Ar<sub>13</sub> underline the capability of the algorithm to find several reaction pathways in one shot.
</p><!--Unmatched element: w:blockFixed--></div>
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We propose a new algorithm to determine reaction paths and test its capability for Ar12 and Ar13 clusters. Its main ingredient is a search for the local minima on a (n−1) dimensional hyperplane (n = dimension of the complete system in Cartesian coordinates) lying perpendicular to the straight line connection between initial and final states. These minima are part of possible reaction paths and are, hence, used as starting points for an uphill search to the next transition state. First, path fragments are obtained from subsequent relaxations starting from these transition states. They can be combined with information from the straight line connection procedure to obtain complete paths. Our test computations for Ar12 and Ar13 clusters prove that PathOpt delivers several reaction paths in one round. © 2013 Wiley Periodicals, Inc.
Knowledge about possible transition and reaction pathways is of utmost importance for the description of many processes like protein folding or complex enzymatic reactions. We propose a new algorithm based on a global optimization in a reduced phase space to locate possible transition states between reactants and products. Investigations for Ar12 and Ar13 underline the capability of the algorithm to find several reaction pathways in one shot.






</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23286" xmlns="http://purl.org/rss/1.0/"><title>Towards quantitative estimates of binding affinities for protein–ligand systems involving large inhibitor compounds: A steered molecular dynamics simulation route</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23286</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Towards quantitative estimates of binding affinities for protein–ligand systems involving large inhibitor compounds: A steered molecular dynamics simulation route</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Paolo Nicolini, Diego Frezzato, Cristina Gellini, Marco Bizzarri, Riccardo Chelli</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-26T02:32:54.858569-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23286</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23286</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23286</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Research Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Understanding binding mechanisms between enzymes and potential inhibitors and quantifying protein<b>–</b>ligand affinities in terms of binding free energy is of primary importance in drug design studies. In this respect, several approaches based on molecular dynamics simulations, often combined with docking techniques, have been exploited to investigate the physicochemical properties of complexes of pharmaceutical interest. Even if the geometric properties of a modeled protein<b>–</b>ligand complex can be well predicted by computational methods, it is still challenging to rank with chemical accuracy a series of ligand analogues in a consistent way. In this article, we face this issue calculating relative binding free energies of a focal adhesion kinase, an important target for the development of anticancer drugs, with pyrrolopyrimidine-based ligands having different inhibitory power. To this aim, we employ steered molecular dynamics simulations combined with nonequilibrium work theorems for free energy calculations. This technique proves very powerful when a series of ligand analogues is considered, allowing one to tackle estimation of protein<b>–</b>ligand relative binding free energies in a reasonable time. In our cases, the calculated binding affinities are comparable with those recovered from experiments by exploiting the Michaelis<b>–</b>Menten mechanism with a competitive inhibitor.</p></div>
<a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/jcc.23286/asset/image_m/jcc23286-toc-0001-m.png?v=1&amp;s=c684532508183211a2e1c2c093b0c692a152c4e8" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23286/asset/image_n/jcc23286-toc-0001.png?v=1&amp;s=c36b5d6e98e20b5909e7cc80f0426e84ebd1d1a3"/></a>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Relative binding free energies of protein–ligand complexes formed by a focal adhesion kinase and various pyrrolopyrimidine-based compounds are calculated by means of steered molecular dynamics simulations. Nonequilibrium trajectories are analyzed using the Jarzynski equality for free energy calculations.
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Understanding binding mechanisms between enzymes and potential inhibitors and quantifying protein–ligand affinities in terms of binding free energy is of primary importance in drug design studies. In this respect, several approaches based on molecular dynamics simulations, often combined with docking techniques, have been exploited to investigate the physicochemical properties of complexes of pharmaceutical interest. Even if the geometric properties of a modeled protein–ligand complex can be well predicted by computational methods, it is still challenging to rank with chemical accuracy a series of ligand analogues in a consistent way. In this article, we face this issue calculating relative binding free energies of a focal adhesion kinase, an important target for the development of anticancer drugs, with pyrrolopyrimidine-based ligands having different inhibitory power. To this aim, we employ steered molecular dynamics simulations combined with nonequilibrium work theorems for free energy calculations. This technique proves very powerful when a series of ligand analogues is considered, allowing one to tackle estimation of protein–ligand relative binding free energies in a reasonable time. In our cases, the calculated binding affinities are comparable with those recovered from experiments by exploiting the Michaelis–Menten mechanism with a competitive inhibitor.
Relative binding free energies of protein–ligand complexes formed by a focal adhesion kinase and various pyrrolopyrimidine-based compounds are calculated by means of steered molecular dynamics simulations. Nonequilibrium trajectories are analyzed using the Jarzynski equality for free energy calculations.





</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23292" xmlns="http://purl.org/rss/1.0/"><title>PHAISTOS: A framework for Markov chain Monte Carlo simulation and inference of protein structure</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23292</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">PHAISTOS: A framework for Markov chain Monte Carlo simulation and inference of protein structure</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Wouter Boomsma, Jes Frellsen, Tim Harder, Sandro Bottaro, Kristoffer E. Johansson, Pengfei Tian, Kasper Stovgaard, Christian Andreetta, Simon Olsson, Jan B. Valentin, Lubomir D. Antonov, Anders S. Christensen, Mikael Borg, Jan H. Jensen, Kresten Lindorff-Larsen, Jesper Ferkinghoff-Borg, Thomas Hamelryck</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-26T02:14:07.710106-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23292</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23292</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23292</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Software News and Updates</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>We present a new software framework for Markov chain Monte Carlo sampling for simulation, prediction, and inference of protein structure. The software package contains implementations of recent advances in Monte Carlo methodology, such as efficient local updates and sampling from probabilistic models of local protein structure. These models form a probabilistic alternative to the widely used fragment and rotamer libraries. Combined with an easily extendible software architecture, this makes PHAISTOS well suited for Bayesian inference of protein structure from sequence and/or experimental data. Currently, two force-fields are available within the framework: PROFASI and OPLS-AA/L, the latter including the generalized Born surface area solvent model. A flexible command-line and configuration-file interface allows users quickly to set up simulations with the desired configuration. PHAISTOS is released under the GNU General Public License v3.0. Source code and documentation are freely available from <!--TODO: clickthrough URL--><a href="http://phaistos.sourceforge.net" title="Link to external resource: http://phaistos.sourceforge.net">http://phaistos.sourceforge.net</a>. The software is implemented in C++ and has been tested on Linux and OSX platforms. © 2013 Wiley Periodicals, Inc.</p></div>
<a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/jcc.23292/asset/image_m/jcc23292-toc-0001-m.png?v=1&amp;s=7294095138fca8074aca32193b03c761332612f0" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23292/asset/image_n/jcc23292-toc-0001.png?v=1&amp;s=90b918d06c99ea1f9f25beda4961fe158496c7ee"/></a>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>We present a new software package for simulation and inference of protein structure. The PHAISTOS framework contains a range of novel sampling techniques and probabilistic models, constituting a versatile toolkit for efficient simulations of protein structure. The package provides tools for a variety of tasks, including reversible folding simulations and probabilistic inference of protein structure from experimental data. The source code is released under an open source license, and full documentation is available online.
</p><!--Unmatched element: w:blockFixed--></div>
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We present a new software framework for Markov chain Monte Carlo sampling for simulation, prediction, and inference of protein structure. The software package contains implementations of recent advances in Monte Carlo methodology, such as efficient local updates and sampling from probabilistic models of local protein structure. These models form a probabilistic alternative to the widely used fragment and rotamer libraries. Combined with an easily extendible software architecture, this makes PHAISTOS well suited for Bayesian inference of protein structure from sequence and/or experimental data. Currently, two force-fields are available within the framework: PROFASI and OPLS-AA/L, the latter including the generalized Born surface area solvent model. A flexible command-line and configuration-file interface allows users quickly to set up simulations with the desired configuration. PHAISTOS is released under the GNU General Public License v3.0. Source code and documentation are freely available from http://phaistos.sourceforge.net. The software is implemented in C++ and has been tested on Linux and OSX platforms. © 2013 Wiley Periodicals, Inc.
We present a new software package for simulation and inference of protein structure. The PHAISTOS framework contains a range of novel sampling techniques and probabilistic models, constituting a versatile toolkit for efficient simulations of protein structure. The package provides tools for a variety of tasks, including reversible folding simulations and probabilistic inference of protein structure from experimental data. The source code is released under an open source license, and full documentation is available online.






</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23287" xmlns="http://purl.org/rss/1.0/"><title>Parameters for molecular dynamics simulations of iron-sulfur proteins</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23287</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Parameters for molecular dynamics simulations of iron-sulfur proteins</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Alexandra T. P. Carvalho, Ana F. S. Teixeira,, Maria J. Ramos</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-23T01:42:03.771719-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23287</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23287</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23287</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Iron-sulfur proteins involved in electron transfer reactions have finely tuned redox potentials, which allow them to be highly efficient and specific. Factors such as metal center solvent exposure, interaction with charged residues, or hydrogen bonds between the ligand residues and amide backbone groups have all been pointed out to cause such specific redox potentials. Here, we derived parameters compatible with the AMBER force field for the metal centers of iron-sulfur proteins and applied them in the molecular dynamics simulations of three iron-sulfur proteins. We used density-functional theory (DFT) calculations and Seminario's method for the parameterization. Parameter validation was obtained by matching structures and normal frequencies at the quantum mechanics and molecular mechanics levels of theory. Having guaranteed a correct representation of the protein coordination spheres, the amide H-bonds and the water exposure to the ligands were analyzed. Our results for the pattern of interactions with the metal centers are consistent to those obtained by nuclear magnetic resonance spectroscopy (NMR) experiments and DFT calculations, allowing the application of molecular dynamics to the study of those proteins. © 2013 Wiley Periodicals, Inc.</p></div>
<a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/jcc.23287/asset/image_m/mgra001.jpg?v=1&amp;s=d28b0f3be41184d8ece0fd7095b97068a4f56094" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23287/asset/image_n/ngra001.jpg?v=1&amp;s=621a5ffd21e378efd6923e417c3fb042b9bf0afd"/></a>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Iron Iron-sulfur proteins have finely tuned redox potentials, which allow them to be highly efficient and specific. Here, we derived bonded parameters compatible with the AMBER force field for three metal centers and performed molecular dynamics simulations on three proteins. Our results for the pattern of interactions with the metal centers are consistent to those obtained by NMR experiments and DFT density functional theory calculations, allowing the application of molecular dynamics to the study of those proteins. </p><!--Unmatched element: w:blockFixed--></div>
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Iron-sulfur proteins involved in electron transfer reactions have finely tuned redox potentials, which allow them to be highly efficient and specific. Factors such as metal center solvent exposure, interaction with charged residues, or hydrogen bonds between the ligand residues and amide backbone groups have all been pointed out to cause such specific redox potentials. Here, we derived parameters compatible with the AMBER force field for the metal centers of iron-sulfur proteins and applied them in the molecular dynamics simulations of three iron-sulfur proteins. We used density-functional theory (DFT) calculations and Seminario's method for the parameterization. Parameter validation was obtained by matching structures and normal frequencies at the quantum mechanics and molecular mechanics levels of theory. Having guaranteed a correct representation of the protein coordination spheres, the amide H-bonds and the water exposure to the ligands were analyzed. Our results for the pattern of interactions with the metal centers are consistent to those obtained by nuclear magnetic resonance spectroscopy (NMR) experiments and DFT calculations, allowing the application of molecular dynamics to the study of those proteins. © 2013 Wiley Periodicals, Inc.
Iron Iron-sulfur proteins have finely tuned redox potentials, which allow them to be highly efficient and specific. Here, we derived bonded parameters compatible with the AMBER force field for three metal centers and performed molecular dynamics simulations on three proteins. Our results for the pattern of interactions with the metal centers are consistent to those obtained by NMR experiments and DFT density functional theory calculations, allowing the application of molecular dynamics to the study of those proteins. 






</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23296" xmlns="http://purl.org/rss/1.0/"><title>Dynamics and structural changes of small water clusters on ionization</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23296</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Dynamics and structural changes of small water clusters on ionization</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Han Myoung Lee, Kwang S. Kim</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-22T09:32:28.701836-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23296</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23296</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23296</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Despite utmost importance in understanding water ionization process, reliable theoretical results of structural changes and molecular dynamics (MD) of water clusters on ionization have hardly been reported yet. Here, we investigate the water cations [(H<sub>2</sub>O)<sub><em>n</em> = 2–6</sub><sup>+</sup>] with density functional theory (DFT), Möller–Plesset second-order perturbation theory (MP2), and coupled cluster theory with single, double, and perturbative triple excitations [CCSD(T)]. The complete basis set limits of interaction energies at the CCSD(T) level are reported, and the geometrical structures, electronic properties, and infrared spectra are investigated. The characteristics of structures and spectra of the water cluster cations reflect the formation of the hydronium cation moiety (H<sub>3</sub>O<sup>+</sup>) and the hydroxyl radical. Although most density functionals fail to predict reasonable energetics of the water cations, some functionals are found to be reliable, in reasonable agreement with high-level <em>ab initio</em> results. To understand the ionization process of water clusters, DFT- and MP2-based Born-Oppenheimer MD (BOMD) simulations are performed on ionization. On ionization, the water clusters tend to have an Eigen-like form with the hydronium cation instead of a Zundel-like form, based on reliable BOMD simulations. For the vertically ionized water hexamer, the relatively stable (H<sub>2</sub>O)<sub>5</sub><sup>+</sup> (5sL4A) cluster tends to form with a detached water molecule (H<sub>2</sub>O). © 2013 Wiley Periodicals, Inc.</p></div>
<a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/jcc.23296/asset/image_m/jcc23296-toc-0001-m.png?v=1&amp;s=90f483950b2e4d9f37dbf6a35deb42e9f20878c8" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23296/asset/image_n/jcc23296-toc-0001.png?v=1&amp;s=435a2b3fba5c103ba98dda1a7f2d901897fe2a4c"/></a>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Water cluster cations can have either the Eigen-like forms or the Zundel-like forms. Based on reliable molecular dynamics simulations, the water clusters tend to have an Eigen-like form with the hydronium cation instead of a Zundel-like form in terms of energetics. For the vertically ionized water hexamer, the relatively stable (H<sub>2</sub>O)<sub>5</sub><sup>+</sup> (5sL4A) cluster tends to form with a detached water molecule (H<sub>2</sub>O).
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Despite utmost importance in understanding water ionization process, reliable theoretical results of structural changes and molecular dynamics (MD) of water clusters on ionization have hardly been reported yet. Here, we investigate the water cations [(H2O)n = 2–6+] with density functional theory (DFT), Möller–Plesset second-order perturbation theory (MP2), and coupled cluster theory with single, double, and perturbative triple excitations [CCSD(T)]. The complete basis set limits of interaction energies at the CCSD(T) level are reported, and the geometrical structures, electronic properties, and infrared spectra are investigated. The characteristics of structures and spectra of the water cluster cations reflect the formation of the hydronium cation moiety (H3O+) and the hydroxyl radical. Although most density functionals fail to predict reasonable energetics of the water cations, some functionals are found to be reliable, in reasonable agreement with high-level ab initio results. To understand the ionization process of water clusters, DFT- and MP2-based Born-Oppenheimer MD (BOMD) simulations are performed on ionization. On ionization, the water clusters tend to have an Eigen-like form with the hydronium cation instead of a Zundel-like form, based on reliable BOMD simulations. For the vertically ionized water hexamer, the relatively stable (H2O)5+ (5sL4A) cluster tends to form with a detached water molecule (H2O). © 2013 Wiley Periodicals, Inc.
Water cluster cations can have either the Eigen-like forms or the Zundel-like forms. Based on reliable molecular dynamics simulations, the water clusters tend to have an Eigen-like form with the hydronium cation instead of a Zundel-like form in terms of energetics. For the vertically ionized water hexamer, the relatively stable (H2O)5+ (5sL4A) cluster tends to form with a detached water molecule (H2O).






</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23298" xmlns="http://purl.org/rss/1.0/"><title>Theoretical characterization and design of small molecule donor material containing naphthodithiophene central unit for efficient organic solar cells</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23298</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Theoretical characterization and design of small molecule donor material containing naphthodithiophene central unit for efficient organic solar cells</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Yu-Ai Duan, Yun Geng, Hai-Bin Li, Jun-Ling Jin, Yong Wu, Zhong-Min Su</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-22T09:31:51.426754-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23298</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23298</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23298</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>To seek for high-performance small molecule donor materials used in heterojunction solar cell, six acceptor–donor–acceptor small molecules based on naphtho[2,3-b:6,7-b′]dithiophene (<b>NDT</b>) units with different acceptor units were designed and characterized using density functional theory and time-dependent density functional theory. Their geometries, electronic structures, photophysical, and charge transport properties have been scrutinized comparing with the reported donor material <b>NDT(TDPP)<sub>2</sub></b> (<b>TDPP</b> = thiophene-capped diketopyrrolopyrrole). The open circuit voltage (<em>V</em><sub>oc</sub>), energetic driving force(Δ<em>E</em><sub>L-L</sub>), and exciton binding energy (<em>E</em><sub>b</sub>) were also provided to give an elementary understanding on their cell performance. The results reveal that the frontier molecular orbitals of <b>3–7</b> match well with the acceptor material <b>PC<sub>61</sub>BM</b>, and compounds <b>3–5</b> were found to exhibit the comparable performances to <b>1</b> and show promising potential in organic solar cells. In particular, comparing with <b>1</b>, system <b>7</b> with naphthobisthiadiazole acceptor unit displays broader absorption spectrum, higher <em>V</em><sub>oc</sub>, lower <em>E</em><sub>b</sub>, and similar carrier mobility. An in-depth insight into the nature of the involved excited states based on transition density matrix and charge density difference indicates that all <em>S</em><sub>1</sub> states are mainly intramolecular charge transfer states with the charge transfer from central <b>NDT</b> unit to bilateral acceptor units, and also imply that the exciton of <b>7</b> can be dissociated easily due to its large extent of the charge transfer. In a word, <b>7</b> maybe superior to <b>1</b> and may act as a promising donor candidate for organic solar cell. © 2013 Wiley Periodicals, Inc.</p></div>
<a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/jcc.23298/asset/image_m/jcc23298-toc-0001-m.png?v=1&amp;s=3acc5c676e18f30511b94d48511110cdca56fbf5" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23298/asset/image_n/jcc23298-toc-0001.png?v=1&amp;s=d4a756f61eade64cb19e62123b0c677aba38aa09"/></a>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p><b>Donor materials</b> with different acceptor units for solar cells were designed and characterized through density functional theory calculations. It is found that <b>7</b> with naphthobisthiadiazole as acceptor fragment may become a high-performance donor due to broad- and red-shifted photoresponse, low exciton binding energies, high open-circuit voltage, and small reorganization energies.
</p><!--Unmatched element: w:blockFixed--></div>
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To seek for high-performance small molecule donor materials used in heterojunction solar cell, six acceptor–donor–acceptor small molecules based on naphtho[2,3-b:6,7-b′]dithiophene (NDT) units with different acceptor units were designed and characterized using density functional theory and time-dependent density functional theory. Their geometries, electronic structures, photophysical, and charge transport properties have been scrutinized comparing with the reported donor material NDT(TDPP)2 (TDPP = thiophene-capped diketopyrrolopyrrole). The open circuit voltage (Voc), energetic driving force(ΔEL-L), and exciton binding energy (Eb) were also provided to give an elementary understanding on their cell performance. The results reveal that the frontier molecular orbitals of 3–7 match well with the acceptor material PC61BM, and compounds 3–5 were found to exhibit the comparable performances to 1 and show promising potential in organic solar cells. In particular, comparing with 1, system 7 with naphthobisthiadiazole acceptor unit displays broader absorption spectrum, higher Voc, lower Eb, and similar carrier mobility. An in-depth insight into the nature of the involved excited states based on transition density matrix and charge density difference indicates that all S1 states are mainly intramolecular charge transfer states with the charge transfer from central NDT unit to bilateral acceptor units, and also imply that the exciton of 7 can be dissociated easily due to its large extent of the charge transfer. In a word, 7 maybe superior to 1 and may act as a promising donor candidate for organic solar cell. © 2013 Wiley Periodicals, Inc.
Donor materials with different acceptor units for solar cells were designed and characterized through density functional theory calculations. It is found that 7 with naphthobisthiadiazole as acceptor fragment may become a high-performance donor due to broad- and red-shifted photoresponse, low exciton binding energies, high open-circuit voltage, and small reorganization energies.






</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23293" xmlns="http://purl.org/rss/1.0/"><title>Existence of dynamic tautomerism and divalent N(I) character in N-(pyridin-2-yl)thiazol-2-amine</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23293</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Existence of dynamic tautomerism and divalent N(I) character in N-(pyridin-2-yl)thiazol-2-amine</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Sonam Bhatia, Yogesh J. Malkhede, Prasad V. Bharatam</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-22T09:30:52.82951-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23293</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23293</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23293</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p><em>N</em>-(Pyridin-2-yl)thiazol-2-amine is a versatile chemical functional unit present in many therapeutically important species. Quantum chemical analysis shows that there are six competitive isomeric structures possible for this class of compounds within a relative energy difference of ∼4 kcal/mol. Some of the isomeric structures possess divalent N(I) character. There appears to be a competition between the thiazole and pyridine groups to accommodate the tautomeric hydrogen, and consequently show electron donating property in the structure with R-N←L representation. Details of electron distribution, tautomeric preferences, protonation energy, and divalent N(I) character, and so on, of this class of compounds are presented in this article. Subsequently, upon protonation, (L→N←L)<sup>⊕</sup> character is clearly evident in these moieties as molecular orbital analysis clearly shows two lone pairs of electrons on the central nitrogen, in this system.</p></div>
<a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/jcc.23293/asset/image_m/jcc23293-toc-0001-m.png?v=1&amp;s=86bda7fe7d1fe8437dc5fb44bc4ebb9fd4cc8c61" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23293/asset/image_n/jcc23293-toc-0001.png?v=1&amp;s=70b391562d06cb1ce6007d64850badfa87ce62c2"/></a>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Quantum chemical calculations using DFT (B3LYP), <em>ab intio</em> methods (MP2), and G2MP2 methods have been carried out to understand the preferences of tautomerization in medicinal relevant <em>N</em>-(pyridin-2-yl)thiazol-2-amine (<b>PTA</b>) scaffolds. <b>PTA-P1</b> is the most preferred isomer for this class of compounds. It shows high proton affinity (∼235 kcal/mol) and gets converted into <b>PTA-P1</b>. Electronic structure analysis of <b>PTA-P1</b> shows that this compound belongs to divalent N(I) of species; characterized by two lone pairs of electrons- π and σ type localized on the central nitrogen. Thus, the form <b>PTA-P1</b> is labeled with (L→N←L)<sup>⊕</sup> character. © 2013 Wiley Periodicals, Inc.
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N-(Pyridin-2-yl)thiazol-2-amine is a versatile chemical functional unit present in many therapeutically important species. Quantum chemical analysis shows that there are six competitive isomeric structures possible for this class of compounds within a relative energy difference of ∼4 kcal/mol. Some of the isomeric structures possess divalent N(I) character. There appears to be a competition between the thiazole and pyridine groups to accommodate the tautomeric hydrogen, and consequently show electron donating property in the structure with R-N←L representation. Details of electron distribution, tautomeric preferences, protonation energy, and divalent N(I) character, and so on, of this class of compounds are presented in this article. Subsequently, upon protonation, (L→N←L)⊕ character is clearly evident in these moieties as molecular orbital analysis clearly shows two lone pairs of electrons on the central nitrogen, in this system.
Quantum chemical calculations using DFT (B3LYP), ab intio methods (MP2), and G2MP2 methods have been carried out to understand the preferences of tautomerization in medicinal relevant N-(pyridin-2-yl)thiazol-2-amine (PTA) scaffolds. PTA-P1 is the most preferred isomer for this class of compounds. It shows high proton affinity (∼235 kcal/mol) and gets converted into PTA-P1. Electronic structure analysis of PTA-P1 shows that this compound belongs to divalent N(I) of species; characterized by two lone pairs of electrons- π and σ type localized on the central nitrogen. Thus, the form PTA-P1 is labeled with (L→N←L)⊕ character. © 2013 Wiley Periodicals, Inc.






</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23297" xmlns="http://purl.org/rss/1.0/"><title>An efficient fluctuating charge model for transition metal complexes</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23297</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">An efficient fluctuating charge model for transition metal complexes</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Peter Comba, Bodo Martin, Avik Sanyal</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-22T09:30:40.893888-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23297</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23297</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23297</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>A fluctuating charge model for transition metal complexes, based on the Hirshfeld partitioning scheme, spectroscopic energy data from the NIST Atomic Spectroscopy Database and the electronegativity equalization approach, has been developed and parameterized for organic ligands and their high- and low-spin Fe<sup>II</sup> and Fe<sup>III</sup>, low-spin Co<sup>III</sup> and Cu<sup>II</sup> complexes, using atom types defined in the Momec force field. Based on large training sets comprising a variety of transition metal complexes, a general parameter set has been developed and independently validated which allows the efficient computation of geometry-dependent charge distributions in the field of transition metal coordination compounds. © 2013 Wiley Periodicals, Inc.</p></div>
<a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/jcc.23297/asset/image_m/jcc23297-toc-0001-m.png?v=1&amp;s=5f74b6418627587aedcc9d325165b6a2e7b4f48b" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23297/asset/image_n/jcc23297-toc-0001.png?v=1&amp;s=d4be2889b428caf11694b15938d03fca16e55bad"/></a>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>An efficient fluctuating charge model for of transition metal complexes, based on the Hirshfeld partitioning scheme, has been developed and validated.
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A fluctuating charge model for transition metal complexes, based on the Hirshfeld partitioning scheme, spectroscopic energy data from the NIST Atomic Spectroscopy Database and the electronegativity equalization approach, has been developed and parameterized for organic ligands and their high- and low-spin FeII and FeIII, low-spin CoIII and CuII complexes, using atom types defined in the Momec force field. Based on large training sets comprising a variety of transition metal complexes, a general parameter set has been developed and independently validated which allows the efficient computation of geometry-dependent charge distributions in the field of transition metal coordination compounds. © 2013 Wiley Periodicals, Inc.
An efficient fluctuating charge model for of transition metal complexes, based on the Hirshfeld partitioning scheme, has been developed and validated.






</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23299" xmlns="http://purl.org/rss/1.0/"><title>IMSPeptider, a computational peptide collision cross-section area calculator based on a novel molecular dynamics simulation protocol</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23299</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">IMSPeptider, a computational peptide collision cross-section area calculator based on a novel molecular dynamics simulation protocol</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Ranieri V. de Carvalho, Daniel Lopez-Ferrer, Katia S. Guimarães, Roberto D. Lins</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-22T09:30:23.537494-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23299</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23299</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23299</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Introduction of ion mobility mass spectrometry (IMS/MS) into the proteomic workflow provides an orthogonal separation to the widely used LC-MS platforms. IMS also provides structural information that could facilitate peptide identification. However, the lack of tools capable of predictive power in a high-throughput fashion makes peptide global profiling quite challenging. To target this issue, a computational workflow was developed based on biophysical principles to predict the collision cross-section area (CCS) of peptides as measured from IMS/MS experiments. Hosted on a web server, it allows the user to input a primary sequence (query) and retrieve information on peptide structure, sequence, and corresponding CCS. The current version is designed to identify peptide sequences up to 23 residues in length, in its higher charge state, based on a match of the molecule <em>m</em>/<em>z</em> and CCS. The protocol was validated against a 128-sequences-dataset and CCS predicted within 2.8% average error. © 2013 Wiley Periodicals, Inc.</p></div>
<a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/jcc.23299/asset/image_m/jcc23299-toc-0001-m.png?v=1&amp;s=4edc09d79f1cee3091dad5c085552e48d46d3074" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23299/asset/image_n/jcc23299-toc-0001.png?v=1&amp;s=33909a1bdcd5b337dbb59010711464055a76cfc2"/></a>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>The lack of tools capable of predictive power in a high throughput fashion makes peptide global profiling quite challenging. To target this issue, a computational workflow was developed based on biophysical principles to predict the collision cross-section area of peptides as measured from ion mobility mass spectrometry experiments. Hosted on a web server, it allows the user to input a primary sequence (query) and retrieve information on peptide structure, sequence, and corresponding collision cross-section area.
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Introduction of ion mobility mass spectrometry (IMS/MS) into the proteomic workflow provides an orthogonal separation to the widely used LC-MS platforms. IMS also provides structural information that could facilitate peptide identification. However, the lack of tools capable of predictive power in a high-throughput fashion makes peptide global profiling quite challenging. To target this issue, a computational workflow was developed based on biophysical principles to predict the collision cross-section area (CCS) of peptides as measured from IMS/MS experiments. Hosted on a web server, it allows the user to input a primary sequence (query) and retrieve information on peptide structure, sequence, and corresponding CCS. The current version is designed to identify peptide sequences up to 23 residues in length, in its higher charge state, based on a match of the molecule m/z and CCS. The protocol was validated against a 128-sequences-dataset and CCS predicted within 2.8% average error. © 2013 Wiley Periodicals, Inc.
The lack of tools capable of predictive power in a high throughput fashion makes peptide global profiling quite challenging. To target this issue, a computational workflow was developed based on biophysical principles to predict the collision cross-section area of peptides as measured from ion mobility mass spectrometry experiments. Hosted on a web server, it allows the user to input a primary sequence (query) and retrieve information on peptide structure, sequence, and corresponding collision cross-section area.






</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23282" xmlns="http://purl.org/rss/1.0/"><title>Modeling peptide binding to anionic membrane pores</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23282</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Modeling peptide binding to anionic membrane pores</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Yi He, Lidia Prieto, Themis Lazaridis</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-11T07:34:04.686456-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23282</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23282</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23282</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Peptide-induced pore formation in membranes can be dissected into two steps: pore formation and peptide binding to the pore. A computational method is proposed to study the second step in anionic membranes. The electrostatic potential is obtained from numerical solutions to the Poisson–Boltzmann equation and is then used in conjunction with IMM1 (implicit membrane model 1). A double charge layer model is used to incorporate the effects of the membrane dipole potential. Inhomogeneity of the charge density in the pore, characterized by explicit membrane simulations of toroidal pores, is included in the model. This approach was applied to two extensively studied peptides, magainin and melittin. In agreement with previous work, binding to toroidal pores is more favorable than binding to the flat membrane. The dependence of binding energy on anionic content exhibits different patterns for the two peptides, in correlation with the different lipid selectivity that has been observed experimentally. © 2013 Wiley Periodicals, Inc.</p></div>
<a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/jcc.23282/asset/image_m/mgra001.jpg?v=1&amp;s=d2a2aef82d95afc980062ee1ecb402023bd258da" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23282/asset/image_n/ngra001.jpg?v=1&amp;s=38c3b510e1a0c94d6667dfdb501df7f0620db46e"/></a>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Antimicrobial peptides are thought to kill bacteria by forming pores in their membranes but their selectivity towards bacterial membranes is not fully understood. An approach is developed to study binding of peptides to anionic membrane pores by combining the electrostatic potential obtained from solution of the Poisson–Boltzmann with the IMM1 implicit membrane model. The binding of two cationic peptides, magainin and melittin, to a pore displays different dependence on anionic content. This correlates with the observed selectivity of these peptides towards zwitterionic and anionic bilayers. </p><!--Unmatched element: w:blockFixed--></div>
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Peptide-induced pore formation in membranes can be dissected into two steps: pore formation and peptide binding to the pore. A computational method is proposed to study the second step in anionic membranes. The electrostatic potential is obtained from numerical solutions to the Poisson–Boltzmann equation and is then used in conjunction with IMM1 (implicit membrane model 1). A double charge layer model is used to incorporate the effects of the membrane dipole potential. Inhomogeneity of the charge density in the pore, characterized by explicit membrane simulations of toroidal pores, is included in the model. This approach was applied to two extensively studied peptides, magainin and melittin. In agreement with previous work, binding to toroidal pores is more favorable than binding to the flat membrane. The dependence of binding energy on anionic content exhibits different patterns for the two peptides, in correlation with the different lipid selectivity that has been observed experimentally. © 2013 Wiley Periodicals, Inc.
Antimicrobial peptides are thought to kill bacteria by forming pores in their membranes but their selectivity towards bacterial membranes is not fully understood. An approach is developed to study binding of peptides to anionic membrane pores by combining the electrostatic potential obtained from solution of the Poisson–Boltzmann with the IMM1 implicit membrane model. The binding of two cationic peptides, magainin and melittin, to a pore displays different dependence on anionic content. This correlates with the observed selectivity of these peptides towards zwitterionic and anionic bilayers. 






</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23291" xmlns="http://purl.org/rss/1.0/"><title>Erratum: A convective replica-exchange method for sampling new energy basins</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23291</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Erratum: A convective replica-exchange method for sampling new energy basins</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Yannick G. Spill, Guillaume Bouvier, Michael Nilges</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-08T00:36:17.390691-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23291</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23291</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23291</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Erratum</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[]]></content:encoded><description/></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23288" xmlns="http://purl.org/rss/1.0/"><title>Relating Trp-Glu dipeptide fluorescence to molecular conformation: The role of the discrete chi 1 and chi 2 angles</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23288</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Relating Trp-Glu dipeptide fluorescence to molecular conformation: The role of the discrete chi 1 and chi 2 angles</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Azaria Solomon Eisenberg, Laura J. Juszczak</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-08T00:36:06.157826-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23288</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23288</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23288</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Molecular dynamics (MD), coupled with fluorescence data for charged dipeptides of tryptophanyl glutamic acid (Trp-Glu), reveal a detailed picture of how specific conformation affects fluorescence. Fluorescence emission spectra and time-resolved emission measurements have been collected for all four charged species. MD simulations 20 to 30 ns in length have also been carried out for the Trp-Glu species, as simulation provides aqueous phase conformational data that can be correlated with the fluorescence data. The calculations show that each dipeptide species is characterized by a similar set of six, discrete Chi 1, Chi 2 dihedral angle pairs. The preferred Chi 1 angles—60°, 180°, and 300°—play the significant role in positioning the terminal amine relative to the indole ring. A Chi 1 angle of 60° results in the arching of the backbone over the indole ring and no interaction of the ring with the terminal amine. Chi 1 values of 180° and 300° result in an extension of the backbone away from the indole ring and a NH<sub>3</sub> cation-π interaction with indole. This interaction is believed responsible for charge transfer quenching. Two fluorescence lifetimes and their corresponding amplitudes correlate with the Chi 1 angle probability distribution for all four charged Trp-Glu dipeptides. Fluorescence emission band maxima are also consistent with the proposed pattern of terminal amine cation quenching of fluorescence. © 2013 Wiley Periodicals, Inc.</p></div>
<a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/jcc.23288/asset/image_m/mgra001.jpg?v=1&amp;s=fd9372d530a5ef9c8cbd89cf1e7f2913aa9de4c1" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23288/asset/image_n/ngra001.jpg?v=1&amp;s=e7968334bc42a1fb6755e2633a27a12548f00f57"/></a>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Molecular dynamics simulation reveals the effect of the Trp-Glu charge state on dipeptide conformation preferences. Two general conformations are found: one where the backbone stretches away from the indole ring, shown here. The consequence of a ‘backbone stretched’ conformation is noncovalent interaction between the terminal amine cation and indole ring, as illustrated here. Using this and other theoretical data, trends in tryptophan fluorescence maxima and lifetimes for different dipeptide species can be explained. </p><!--Unmatched element: w:blockFixed--></div>
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Molecular dynamics (MD), coupled with fluorescence data for charged dipeptides of tryptophanyl glutamic acid (Trp-Glu), reveal a detailed picture of how specific conformation affects fluorescence. Fluorescence emission spectra and time-resolved emission measurements have been collected for all four charged species. MD simulations 20 to 30 ns in length have also been carried out for the Trp-Glu species, as simulation provides aqueous phase conformational data that can be correlated with the fluorescence data. The calculations show that each dipeptide species is characterized by a similar set of six, discrete Chi 1, Chi 2 dihedral angle pairs. The preferred Chi 1 angles—60°, 180°, and 300°—play the significant role in positioning the terminal amine relative to the indole ring. A Chi 1 angle of 60° results in the arching of the backbone over the indole ring and no interaction of the ring with the terminal amine. Chi 1 values of 180° and 300° result in an extension of the backbone away from the indole ring and a NH3 cation-π interaction with indole. This interaction is believed responsible for charge transfer quenching. Two fluorescence lifetimes and their corresponding amplitudes correlate with the Chi 1 angle probability distribution for all four charged Trp-Glu dipeptides. Fluorescence emission band maxima are also consistent with the proposed pattern of terminal amine cation quenching of fluorescence. © 2013 Wiley Periodicals, Inc.
Molecular dynamics simulation reveals the effect of the Trp-Glu charge state on dipeptide conformation preferences. Two general conformations are found: one where the backbone stretches away from the indole ring, shown here. The consequence of a ‘backbone stretched’ conformation is noncovalent interaction between the terminal amine cation and indole ring, as illustrated here. Using this and other theoretical data, trends in tryptophan fluorescence maxima and lifetimes for different dipeptide species can be explained. 






</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23285" xmlns="http://purl.org/rss/1.0/"><title>Finding optimal finite field strengths allowing for a maximum of precision in the calculation of polarizabilities and hyperpolarizabilities</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23285</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Finding optimal finite field strengths allowing for a maximum of precision in the calculation of polarizabilities and hyperpolarizabilities</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Ahmed A. K. Mohammed, Peter A. Limacher, Benoît Champagne</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-04T08:13:42.554392-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23285</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23285</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23285</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>The finite field method, widely used for the calculation of static dipole polarizabilities or the first and second hyperpolarizabilities of molecules and polymers, is thoroughly explored. The application of different field strengths and the impact on the precision of the calculations were investigated. Borders could be defined and characterized, establishing a range of feasible field strengths that guarantee reliable numerical results. The quality of different types of meshes to screen the feasible region is assessed. Extrapolation schemes are presented that reduce the truncation error and allow to increase the precision of finite field calculations by one to three orders of magnitude. © 2013 Wiley Periodicals, Inc.</p></div>
<a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/jcc.23285/asset/image_m/mgra001.jpg?v=1&amp;s=b164227875151b09e90c1493f2e2f439d4215f28" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23285/asset/image_n/ngra001.jpg?v=1&amp;s=7ae80a6e97717f5cf3ecc302f6d67a3da13ae0db"/></a>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>The precision of second hyperpolarizability calculations using the finite field approach can be refined combining the results of several different field strengths. Each entry of a column <em>m</em> is a linear combination of the two adjacent values from the <em>m</em>−1 column. Colored values indicate good precision. The reference value in atomic units is the second hyperpolarizability of neon at the HF/t-aug-cc-pVQZ level of theory. </p><!--Unmatched element: w:blockFixed--></div>
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The finite field method, widely used for the calculation of static dipole polarizabilities or the first and second hyperpolarizabilities of molecules and polymers, is thoroughly explored. The application of different field strengths and the impact on the precision of the calculations were investigated. Borders could be defined and characterized, establishing a range of feasible field strengths that guarantee reliable numerical results. The quality of different types of meshes to screen the feasible region is assessed. Extrapolation schemes are presented that reduce the truncation error and allow to increase the precision of finite field calculations by one to three orders of magnitude. © 2013 Wiley Periodicals, Inc.
The precision of second hyperpolarizability calculations using the finite field approach can be refined combining the results of several different field strengths. Each entry of a column m is a linear combination of the two adjacent values from the m−1 column. Colored values indicate good precision. The reference value in atomic units is the second hyperpolarizability of neon at the HF/t-aug-cc-pVQZ level of theory. 






</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23283" xmlns="http://purl.org/rss/1.0/"><title>Use of ab initio methods for the interpretation of the experimental IR reflectance spectra of crystalline compounds</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23283</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Use of ab initio methods for the interpretation of the experimental IR reflectance spectra of crystalline compounds</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Marco De La Pierre, Cédric Carteret, Roberto Orlando, Roberto Dovesi</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-04T08:13:36.347598-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23283</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23283</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23283</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>It is shown that <em>ab initio</em> simulation can be used as a powerful complementary tool in the interpretation of the experimental reflectance spectra <em>R</em>(ν) of crystalline compounds. Experimental frequencies and intensities are obtained from a best fit of <em>R</em>(ν) with a set of damped harmonic oscillators, whose number and initial position in frequency can dramatically influence the final results, as the parameters are strongly correlated. Computed <em>ab initio</em> values for frequencies and intensities are accurate enough to represent an excellent starting point for the best fit process. Moreover, at variance with respect to experiment, simulation permits to identify all the symmetry allowed modes, also when characterized by low intensity or when close to a very intense peak. Overall, simulation-aided analysis of experimental spectra prevents from classifying combination modes as fundamental modes and permits to discard artifacts due to superposition of bands, background, and noise. Finally, it allows to (almost) completely characterize the set of fundamental modes. © 2013 Wiley Periodicals, Inc.</p></div>
<a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/jcc.23283/asset/image_m/mgra001.jpg?v=1&amp;s=a3b432ff3e3c8a7625b5bc1a516759784d64dae3" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23283/asset/image_n/ngra001.jpg?v=1&amp;s=fbc0d92ee37cd1e7abd80777f717ce6bf33262f0"/></a>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>It is shown how ab initio simulation can be used as a complementary tool for the interpretation of the experimental infrared reflectance spectra of solids. Accurate computed frequencies and intensities are an excellent guess for the best fit process used to extract the corresponding experimental quantities. Most of the symmetry allowed fundamental modes are in this way identified, including low intensity features. Combination modes are characterized, while artifacts due to background/noise are more easily disregarded. </p><!--Unmatched element: w:blockFixed--></div>
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It is shown that ab initio simulation can be used as a powerful complementary tool in the interpretation of the experimental reflectance spectra R(ν) of crystalline compounds. Experimental frequencies and intensities are obtained from a best fit of R(ν) with a set of damped harmonic oscillators, whose number and initial position in frequency can dramatically influence the final results, as the parameters are strongly correlated. Computed ab initio values for frequencies and intensities are accurate enough to represent an excellent starting point for the best fit process. Moreover, at variance with respect to experiment, simulation permits to identify all the symmetry allowed modes, also when characterized by low intensity or when close to a very intense peak. Overall, simulation-aided analysis of experimental spectra prevents from classifying combination modes as fundamental modes and permits to discard artifacts due to superposition of bands, background, and noise. Finally, it allows to (almost) completely characterize the set of fundamental modes. © 2013 Wiley Periodicals, Inc.
It is shown how ab initio simulation can be used as a complementary tool for the interpretation of the experimental infrared reflectance spectra of solids. Accurate computed frequencies and intensities are an excellent guess for the best fit process used to extract the corresponding experimental quantities. Most of the symmetry allowed fundamental modes are in this way identified, including low intensity features. Combination modes are characterized, while artifacts due to background/noise are more easily disregarded. 






</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23278" xmlns="http://purl.org/rss/1.0/"><title>Program fullerene—a software package for constructing and analyzing structures of regular fullerenes</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23278</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Program fullerene—a software package for constructing and analyzing structures of regular fullerenes</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Peter Schwerdtfeger, Lukas Wirz, James Avery</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-04T08:13:17.51261-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23278</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23278</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23278</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Software News and Updates</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p><em>Fullerene</em> (Version 4.4) is a general purpose open-source program that can generate any fullerene isomer, perform topological and graph theoretical analysis, as well as calculate a number of physical and chemical properties. The program creates symmetric planar drawings of the fullerene graph and generates accurate molecular 3D geometries by way of force-field optimization, serving as a good starting point for further quantum theoretical treatments. It includes a number of fullerene-to-fullerene transformations, such as Goldberg–Coxeter transforms, Stone–Wales transforms, Endo–Kroto, Yoshida–Fowler, and Brinkmann–Fowler vertex insertions. The program is written in standard Fortran and C++ and can easily be installed in a Linux or UNIX environment. © 2013 Wiley Periodicals, Inc.</p></div>
<a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/jcc.23278/asset/image_m/mgra001.jpg?v=1&amp;s=d73956cc430076ddd4f9a44c719cb5d1ade81174" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23278/asset/image_n/ngra001.jpg?v=1&amp;s=3ff5fcf9a3dfa5aafa5b30b9b70fb219b370887b"/></a>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p><em>Fullerene</em> is an open-source general purpose program that constructs any fullerene graph, performs topological and physical analyses, and creates accurate 3D fullerene structures through graph theoretical methods and force-field optimizations. It allows for Goldberg–Coxeter transformations, vertex insertions, and Stone–Wales transformations. </p><!--Unmatched element: w:blockFixed--></div>
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Fullerene (Version 4.4) is a general purpose open-source program that can generate any fullerene isomer, perform topological and graph theoretical analysis, as well as calculate a number of physical and chemical properties. The program creates symmetric planar drawings of the fullerene graph and generates accurate molecular 3D geometries by way of force-field optimization, serving as a good starting point for further quantum theoretical treatments. It includes a number of fullerene-to-fullerene transformations, such as Goldberg–Coxeter transforms, Stone–Wales transforms, Endo–Kroto, Yoshida–Fowler, and Brinkmann–Fowler vertex insertions. The program is written in standard Fortran and C++ and can easily be installed in a Linux or UNIX environment. © 2013 Wiley Periodicals, Inc.
Fullerene is an open-source general purpose program that constructs any fullerene graph, performs topological and physical analyses, and creates accurate 3D fullerene structures through graph theoretical methods and force-field optimizations. It allows for Goldberg–Coxeter transformations, vertex insertions, and Stone–Wales transformations. 






</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23284" xmlns="http://purl.org/rss/1.0/"><title>Attractive electron–electron interactions within robust local fitting approximations</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23284</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Attractive electron–electron interactions within robust local fitting approximations</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Patrick Merlot, Thomas Kjærgaard, Trygve Helgaker, Roland Lindh, Francesco Aquilante, Simen Reine, Thomas Bondo Pedersen</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-03T04:23:14.964524-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23284</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23284</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23284</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>An analysis of Dunlap's robust fitting approach reveals that the resulting two-electron integral matrix is not manifestly positive semidefinite when local fitting domains or non-Coulomb fitting metrics are used. We present a highly local approximate method for evaluating four-center two-electron integrals based on the resolution-of-the-identity (RI) approximation and apply it to the construction of the Coulomb and exchange contributions to the Fock matrix. In this pair-atomic resolution-of-the-identity (PARI) approach, atomic-orbital (AO) products are expanded in auxiliary functions centered on the two atoms associated with each product. Numerical tests indicate that in 1% or less of all Hartree–Fock and Kohn–Sham calculations, the indefinite integral matrix causes nonconvergence in the self-consistent-field iterations. In these cases, the two-electron contribution to the total energy becomes negative, meaning that the electronic interaction is effectively attractive, and the total energy is dramatically lower than that obtained with exact integrals. In the vast majority of our test cases, however, the indefiniteness does not interfere with convergence. The total energy accuracy is comparable to that of the standard Coulomb-metric RI method. The speed-up compared with conventional algorithms is similar to the RI method for Coulomb contributions; exchange contributions are accelerated by a factor of up to eight with a triple-zeta quality basis set. A positive semidefinite integral matrix is recovered within PARI by introducing local auxiliary basis functions spanning the full AO product space, as may be achieved by using Cholesky-decomposition techniques. Local completion, however, slows down the algorithm to a level comparable with or below conventional calculations. © 2013 Wiley Periodicals, Inc.</p></div>
<a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/jcc.23284/asset/image_m/mgra001.jpg?v=1&amp;s=8b6f6f966ab6b2a6a8f1ad407fa42f14975b45e1" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23284/asset/image_n/ngra001.jpg?v=1&amp;s=6c556d66b1e24b21452a0c3ff7b726466d6dd007"/></a>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Using robust local fitting procedures to approximate two-electron integrals, self-consistent field iterations may fail to converge as a result of effectively attractive electronic interactions. Convergence is recovered when the negative eigenvalues of the approximate two-electron integral matrix become sufficiently small. This is guaranteed when the auxiliary basis set is locally (near-) complete, which may be achieved using Cholesky-decomposition techniques. </p><!--Unmatched element: w:blockFixed--></div>
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An analysis of Dunlap's robust fitting approach reveals that the resulting two-electron integral matrix is not manifestly positive semidefinite when local fitting domains or non-Coulomb fitting metrics are used. We present a highly local approximate method for evaluating four-center two-electron integrals based on the resolution-of-the-identity (RI) approximation and apply it to the construction of the Coulomb and exchange contributions to the Fock matrix. In this pair-atomic resolution-of-the-identity (PARI) approach, atomic-orbital (AO) products are expanded in auxiliary functions centered on the two atoms associated with each product. Numerical tests indicate that in 1% or less of all Hartree–Fock and Kohn–Sham calculations, the indefinite integral matrix causes nonconvergence in the self-consistent-field iterations. In these cases, the two-electron contribution to the total energy becomes negative, meaning that the electronic interaction is effectively attractive, and the total energy is dramatically lower than that obtained with exact integrals. In the vast majority of our test cases, however, the indefiniteness does not interfere with convergence. The total energy accuracy is comparable to that of the standard Coulomb-metric RI method. The speed-up compared with conventional algorithms is similar to the RI method for Coulomb contributions; exchange contributions are accelerated by a factor of up to eight with a triple-zeta quality basis set. A positive semidefinite integral matrix is recovered within PARI by introducing local auxiliary basis functions spanning the full AO product space, as may be achieved by using Cholesky-decomposition techniques. Local completion, however, slows down the algorithm to a level comparable with or below conventional calculations. © 2013 Wiley Periodicals, Inc.
Using robust local fitting procedures to approximate two-electron integrals, self-consistent field iterations may fail to converge as a result of effectively attractive electronic interactions. Convergence is recovered when the negative eigenvalues of the approximate two-electron integral matrix become sufficiently small. This is guaranteed when the auxiliary basis set is locally (near-) complete, which may be achieved using Cholesky-decomposition techniques. 






</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23280" xmlns="http://purl.org/rss/1.0/"><title>On the Vibrational linear and nonlinear optical properties of compounds involving noble gas atoms: HXeOXeH, HXeOXeF, and FXeOXeF</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23280</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">On the Vibrational linear and nonlinear optical properties of compounds involving noble gas atoms: HXeOXeH, HXeOXeF, and FXeOXeF</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Aggelos Avramopoulos, Heribert Reis, Josep M. Luis, Manthos G. Papadopoulos</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-03T04:22:59.950483-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23280</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23280</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23280</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>The vibrational (hyper)polarizabilities of some selected Xe derivatives are studied in the context of Bishop–Kirtman perturbation theory (BKPT) and numerical finite field methodology. It was found that for this set of rare gas compounds, the static vibrational properties are quite large, in comparison to the corresponding electronic ones, especially those of the second hyperpolarizability. This also holds for the dc-Pockels β(−ω;ω,0), Kerr γ(−ω;ω,0,0) and electric field second harmonic generation γ (−2ω;ω,ω,0) effects, although the computed nuclear relaxation (nr) vibrational contributions are smaller in magnitude than the static ones. HXeOXeH was used to study the effects of electron correlation, basis set, and geometry. Geometry effects were found to lead to noticeable changes of the vibrational and electronic second hyperpolarizability. A limited study of the effect of Xe insertion to the nr vibrational properties is also reported. Assessment of the results revealed that Xe insertion has a remarkable effect on the nr (hyper)polarizabilities. In terms of the BKPT, this is associated with a remarkable increase of the electrical and mechanical anharmonicity terms. The latter is consistent with the anharmonic character of several vibrational modes reported for rare gas compounds. © 2013 Wiley Periodicals, Inc.</p></div>
<a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/jcc.23280/asset/image_m/mgra001.jpg?v=1&amp;s=0261e620c8117aa947c38885c159599eb4696cf1" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23280/asset/image_n/ngra001.jpg?v=1&amp;s=73f0e10fcf4263453eab41e157e1470aa456b09f"/></a>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>The electronic and vibrational (hyper)polarizabilities of some rare gas derivatives, HXeOXeH, HXeOXeF, and FXeOXeF, are reported. All the studied properties were computed by employing state-of-the art quantum chemistry methods. This article discusses certain features associated with the remarkable effect of rare gas atom(s) on the electronic and vibrational nonlinear optical properties. </p><!--Unmatched element: w:blockFixed--></div>
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The vibrational (hyper)polarizabilities of some selected Xe derivatives are studied in the context of Bishop–Kirtman perturbation theory (BKPT) and numerical finite field methodology. It was found that for this set of rare gas compounds, the static vibrational properties are quite large, in comparison to the corresponding electronic ones, especially those of the second hyperpolarizability. This also holds for the dc-Pockels β(−ω;ω,0), Kerr γ(−ω;ω,0,0) and electric field second harmonic generation γ (−2ω;ω,ω,0) effects, although the computed nuclear relaxation (nr) vibrational contributions are smaller in magnitude than the static ones. HXeOXeH was used to study the effects of electron correlation, basis set, and geometry. Geometry effects were found to lead to noticeable changes of the vibrational and electronic second hyperpolarizability. A limited study of the effect of Xe insertion to the nr vibrational properties is also reported. Assessment of the results revealed that Xe insertion has a remarkable effect on the nr (hyper)polarizabilities. In terms of the BKPT, this is associated with a remarkable increase of the electrical and mechanical anharmonicity terms. The latter is consistent with the anharmonic character of several vibrational modes reported for rare gas compounds. © 2013 Wiley Periodicals, Inc.
The electronic and vibrational (hyper)polarizabilities of some rare gas derivatives, HXeOXeH, HXeOXeF, and FXeOXeF, are reported. All the studied properties were computed by employing state-of-the art quantum chemistry methods. This article discusses certain features associated with the remarkable effect of rare gas atom(s) on the electronic and vibrational nonlinear optical properties. 






</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23281" xmlns="http://purl.org/rss/1.0/"><title>Pipek–Mezey localization of occupied and virtual orbitals</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23281</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Pipek–Mezey localization of occupied and virtual orbitals</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Ida-Marie Høyvik, Branislav Jansik, Poul Jørgensen</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-03T01:57:01.226478-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23281</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23281</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23281</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Recent advances in orbital localization algorithms are used to minimize the Pipek–Mezey localization function for both occupied and virtual Hartree–Fock orbitals. Virtual Pipek–Mezey orbitals for large molecular systems have previously not been considered in the literature. For this work, the Pipek–Mezey (PM) localization function is implemented for both the Mulliken and a Löwdin population analysis. The results show that the standard PM localization function (using either Mulliken or Löwdin population analyses) may yield local occupied orbitals, although for some systems the occupied orbitals are only semilocal as compared to state-of-the-art localized occupied orbitals. For the virtual orbitals, a Löwdin population analysis shows improvement in locality compared to a Mulliken population analysis, but for both Mulliken and Löwdin population analyses, the virtual orbitals are seen to be considerably less local compared to state-of-the-art localized orbitals. © 2013 Wiley Periodicals, Inc.</p></div>
<a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/jcc.23281/asset/image_m/mgra001.jpg?v=1&amp;s=b7df86ed55354cb6af2837a7992e6860348b3d95" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23281/asset/image_n/ngra001.jpg?v=1&amp;s=b1b40708f395ae48b71e4f098ab74b007195cdb9"/></a>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Equations needed to employ recent advances in orbital localization algorithms for the Pipek–Mezey (PM) localization function are presented, and used to investigate the locality of both occupied and virtual PM orbitals for large molecular systems. The locality of the occupied orbitals have seen to be generally good, although very system dependent (as displayed by picture of a occupied PM orbital for a graphene sheet plotted using contour 0.003). The virtual PM orbitals are shown to exhibit poor locality. </p><!--Unmatched element: w:blockFixed--></div>
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Recent advances in orbital localization algorithms are used to minimize the Pipek–Mezey localization function for both occupied and virtual Hartree–Fock orbitals. Virtual Pipek–Mezey orbitals for large molecular systems have previously not been considered in the literature. For this work, the Pipek–Mezey (PM) localization function is implemented for both the Mulliken and a Löwdin population analysis. The results show that the standard PM localization function (using either Mulliken or Löwdin population analyses) may yield local occupied orbitals, although for some systems the occupied orbitals are only semilocal as compared to state-of-the-art localized occupied orbitals. For the virtual orbitals, a Löwdin population analysis shows improvement in locality compared to a Mulliken population analysis, but for both Mulliken and Löwdin population analyses, the virtual orbitals are seen to be considerably less local compared to state-of-the-art localized orbitals. © 2013 Wiley Periodicals, Inc.
Equations needed to employ recent advances in orbital localization algorithms for the Pipek–Mezey (PM) localization function are presented, and used to investigate the locality of both occupied and virtual PM orbitals for large molecular systems. The locality of the occupied orbitals have seen to be generally good, although very system dependent (as displayed by picture of a occupied PM orbital for a graphene sheet plotted using contour 0.003). The virtual PM orbitals are shown to exhibit poor locality. 






</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23279" xmlns="http://purl.org/rss/1.0/"><title>Computational design of S-nitrosothiol “Click” reactions</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23279</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Computational design of S-nitrosothiol “Click” reactions</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Marat R. Talipov, Dmitry G. Khomyakov, Ming Xian, Qadir K. Timerghazin</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-03T01:56:46.347664-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23279</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23279</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23279</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Rapid Communication</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>To address a long-standing problem of finding efficient reactions for chemical labeling of protein-based <em>S</em>-nitrosothiols (RSNOs), we computationally explored hitherto unknown (3+2) cycloaddition RSNO reactions with alkynes and alkenes. Nonactivated RSNO cycloaddition reactions have high activation enthalpy (&gt;20 kcal/mol at the CBS-QB3 level) and compete with alternative S<img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8ff.gif" alt="[BOND]"/>N bond insertion pathway. However, the (3+2) cycloaddition reaction barriers can be dramatically lowered by coordination of a Lewis acid to the N atom of the <img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8ff.gif" alt="[BOND]"/>SNO group. To exploit this effect, we propose to use reagents with Lewis acid and a strain-activated carbon–carbon multiple bond linked by a rigid scaffold, which can react with RSNOs with small activation enthalpies (∼5 kcal/mol) and high reaction exothermicities (∼40 kcal/mol). The proposed efficient RSNO cycloaddition reactions can be used for future development of practical RSNO labeling reactions. © 2013 Wiley Periodicals, Inc.</p></div>
<a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/jcc.23279/asset/image_m/mgra001.jpg?v=1&amp;s=e44815128865af336e435339a262ddab20af0ced" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23279/asset/image_n/ngra001.jpg?v=1&amp;s=b112f5601d3f5bd17ad3b38ee3752006cdb60a0c"/></a>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Making <em>S</em>-nitrosothiols click: CBS-QB3 calculations show that <em>N</em>-coordination of a Lewis acid (LA) is all that is necessary for <em>S</em>-nitrosothiols (RSNOs) to undergo efficient (3+2) cycloaddition reactions with activated alkynes or alkenes. We propose that LA-linked reagents may have great potential for labeling unstable protein-based RSNOs, as they are predicted to react with RSNOs with efficiency approaching click-chemistry based reactions. </p><!--Unmatched element: w:blockFixed--></div>
]]></content:encoded><description>

To address a long-standing problem of finding efficient reactions for chemical labeling of protein-based S-nitrosothiols (RSNOs), we computationally explored hitherto unknown (3+2) cycloaddition RSNO reactions with alkynes and alkenes. Nonactivated RSNO cycloaddition reactions have high activation enthalpy (&gt;20 kcal/mol at the CBS-QB3 level) and compete with alternative S<img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8ff.gif" alt="[BOND]"/>N bond insertion pathway. However, the (3+2) cycloaddition reaction barriers can be dramatically lowered by coordination of a Lewis acid to the N atom of the <img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8ff.gif" alt="[BOND]"/>SNO group. To exploit this effect, we propose to use reagents with Lewis acid and a strain-activated carbon–carbon multiple bond linked by a rigid scaffold, which can react with RSNOs with small activation enthalpies (∼5 kcal/mol) and high reaction exothermicities (∼40 kcal/mol). The proposed efficient RSNO cycloaddition reactions can be used for future development of practical RSNO labeling reactions. © 2013 Wiley Periodicals, Inc.
Making S-nitrosothiols click: CBS-QB3 calculations show that N-coordination of a Lewis acid (LA) is all that is necessary for S-nitrosothiols (RSNOs) to undergo efficient (3+2) cycloaddition reactions with activated alkynes or alkenes. We propose that LA-linked reagents may have great potential for labeling unstable protein-based RSNOs, as they are predicted to react with RSNOs with efficiency approaching click-chemistry based reactions. 






</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23270" xmlns="http://purl.org/rss/1.0/"><title>Photodeactivation paths in norbornadiene</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23270</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Photodeactivation paths in norbornadiene</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Ivana Antol</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-03T01:55:40.047074-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23270</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23270</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23270</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>The first high level <em>ab initio</em> quantum-chemical calculations of potential energy surfaces (PESs) for low-lying singlet excited states of norbornadiene in the gas phase are presented. The optimization of the stationary points (minima and conical intersections) and the recalculation of the energies were performed using the multireference configuration interaction with singles (MR-CIS) and the multiconfigurational second-order perturbation (CASPT2) methods, respectively. It was shown that the crossing between valence V<sub>2</sub> and Rydberg R<sub>1</sub> states close to the Franck–Condon (FC) point permits an easy population switch between these states. Also, a new deactivation path in which the doubly excited state with (π<sub>3</sub>)<sup>2</sup> configuration (DE) has a prominent role in photodeactivation from the R<sub>1</sub> state due to the R<sub>1</sub>/DE and the DE/V<sub>1</sub> conical intersections very close to the R<sub>1</sub> and DE minima, respectively, was proposed. Subsequent deactivation from the V<sub>1</sub> to the ground state goes through an Olivucci–Robb-type conical intersection that adopts a rhombic distorted geometry. The deactivation path has negligible barriers, thereby making ultrafast radiationless decay to the ground state possible. © 2013 Wiley Periodicals, Inc.</p></div>
<a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/jcc.23270/asset/image_m/mgra001.jpg?v=1&amp;s=4e21752f3b7ef3b0d81b9f6af476657ad082c617" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23270/asset/image_n/ngra001.jpg?v=1&amp;s=a2f79e1ac83377bf89c22351a7828f06be509287"/></a>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>The first high level quantum-chemical calculations of norbornadiene's singlet excited-state PE surfaces revealed a new photodeactivation path in which the dark doubly excited state has a prominent role due to the R<sub>1</sub>/DE and DE/V<sub>1</sub> conical intersections. </p><!--Unmatched element: w:blockFixed--></div>
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The first high level ab initio quantum-chemical calculations of potential energy surfaces (PESs) for low-lying singlet excited states of norbornadiene in the gas phase are presented. The optimization of the stationary points (minima and conical intersections) and the recalculation of the energies were performed using the multireference configuration interaction with singles (MR-CIS) and the multiconfigurational second-order perturbation (CASPT2) methods, respectively. It was shown that the crossing between valence V2 and Rydberg R1 states close to the Franck–Condon (FC) point permits an easy population switch between these states. Also, a new deactivation path in which the doubly excited state with (π3)2 configuration (DE) has a prominent role in photodeactivation from the R1 state due to the R1/DE and the DE/V1 conical intersections very close to the R1 and DE minima, respectively, was proposed. Subsequent deactivation from the V1 to the ground state goes through an Olivucci–Robb-type conical intersection that adopts a rhombic distorted geometry. The deactivation path has negligible barriers, thereby making ultrafast radiationless decay to the ground state possible. © 2013 Wiley Periodicals, Inc.
The first high level quantum-chemical calculations of norbornadiene's singlet excited-state PE surfaces revealed a new photodeactivation path in which the dark doubly excited state has a prominent role due to the R1/DE and DE/V1 conical intersections. 






</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23277" xmlns="http://purl.org/rss/1.0/"><title>Computation of magnetic circular dichroism by sum over states summations</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23277</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Computation of magnetic circular dichroism by sum over states summations</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Petr Štěpánek, Petr Bouř</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-23T03:54:11.163365-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23277</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23277</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23277</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Magnetic circular dichroism (MCD) spectroscopy has been established as a convenient method to study electronic structure, in particular for small symmetric organic molecules. Newer applications on more complex systems are additionally stimulated by the latest availability of precise quantum-chemical techniques for the spectral simulations. In this work, a sum over states (SOS) summation is reexamined as an alternative to the derivative techniques for the MCD modeling. Unlike in previous works, the excited electronic states are calculated by the time-dependent density functional theory (TDDFT). A gradient formulation of the MCD intensities is also proposed, less dependent on the origin choice than the standard expressions. The dependencies of the results on the basis set, number of electronic states, and coordinate origin are tested on model examples, including large symmetric molecules with degenerate electronic states. The results suggest that the SOS/TDDFT approach is a viable and accurate technique for spectral simulation. It may even considerably reduce the computational time, if compared with the traditional MCD computational procedures based on the response theory. © 2013 Wiley Periodicals, Inc.</p></div>
<a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/jcc.23277/asset/image_m/mgra001.jpg?v=1&amp;s=c08690773d66cf41197cb039746d61212196653d" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23277/asset/image_n/ngra001.jpg?v=1&amp;s=e14b100dcf15a264b715be5d4d99162ed72d2d2d"/></a>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>The spectroscopy of magnetic circular dichroism has been lately profiting from the possibility to calculate accurately the spectra within the DFT and response theories. Surprisingly, we found that also the DFT sum over state path is a viable alternate approach, which under certain circumstances even significantly speeds up the spectral modeling. </p><!--Unmatched element: w:blockFixed--></div>
]]></content:encoded><description>

Magnetic circular dichroism (MCD) spectroscopy has been established as a convenient method to study electronic structure, in particular for small symmetric organic molecules. Newer applications on more complex systems are additionally stimulated by the latest availability of precise quantum-chemical techniques for the spectral simulations. In this work, a sum over states (SOS) summation is reexamined as an alternative to the derivative techniques for the MCD modeling. Unlike in previous works, the excited electronic states are calculated by the time-dependent density functional theory (TDDFT). A gradient formulation of the MCD intensities is also proposed, less dependent on the origin choice than the standard expressions. The dependencies of the results on the basis set, number of electronic states, and coordinate origin are tested on model examples, including large symmetric molecules with degenerate electronic states. The results suggest that the SOS/TDDFT approach is a viable and accurate technique for spectral simulation. It may even considerably reduce the computational time, if compared with the traditional MCD computational procedures based on the response theory. © 2013 Wiley Periodicals, Inc.
The spectroscopy of magnetic circular dichroism has been lately profiting from the possibility to calculate accurately the spectra within the DFT and response theories. Surprisingly, we found that also the DFT sum over state path is a viable alternate approach, which under certain circumstances even significantly speeds up the spectral modeling. 






</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23336" xmlns="http://purl.org/rss/1.0/"><title>Cover Image, Volume 34, Issue 16</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23336</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Cover Image, Volume 34, Issue 16</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-09T09:49:58.444615-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23336</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23336</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23336</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Cover Image</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">i</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">ii</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/jcc.23336/asset/image_m/jcc23336-fig-0001-m.png?v=1&amp;s=f70e485b125a1987ccc59ef1d7d07accf4f402f4" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23336/asset/image_n/jcc23336-fig-0001.png?v=1&amp;s=f037564d119a2ca8952ce67ae495b2cbab203fe7"/></a>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><!--Unmatched element: w:blockFixed--><p> NBO 6.0, the next generation in natural bond orbital methods, is released by Frank Weinhold, Eric Glendening, and Clark Landis <!--TODO: clickthrough URL--><a href="http://dx.doi.org/10.1002/jcc.23266" title="Link to external resource: http://dx.doi.org/10.1002/jcc.23266">on page 1429</a>. NBO 6.0 includes link-free connectivity for interfaces to popular electronic structure programs, new methods of analysis, and numerous algorithmic enhancements. The cover image is made with the NBOView 2.0 program and shows the sigma-type, 3-center/2-electron bonding NBO of the cyclobutenyl cation that arises from the strong overlap of the vacant valence orbital at C1 with the C2–C3 bond. Automated multicenter bond searches are one of the many new features of the NBO program.</p></div>
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 NBO 6.0, the next generation in natural bond orbital methods, is released by Frank Weinhold, Eric Glendening, and Clark Landis on page 1429. NBO 6.0 includes link-free connectivity for interfaces to popular electronic structure programs, new methods of analysis, and numerous algorithmic enhancements. The cover image is made with the NBOView 2.0 program and shows the sigma-type, 3-center/2-electron bonding NBO of the cyclobutenyl cation that arises from the strong overlap of the vacant valence orbital at C1 with the C2–C3 bond. Automated multicenter bond searches are one of the many new features of the NBO program.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23337" xmlns="http://purl.org/rss/1.0/"><title>Inside Cover, Volume 34, Issue 16</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23337</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Inside Cover, Volume 34, Issue 16</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-09T09:49:58.444615-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23337</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23337</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23337</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Cover Image</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">iii</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">iv</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[<a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/jcc.23337/asset/image_m/jcc23337-fig-0001-m.png?v=1&amp;s=88ed7bd42b441ef3d985306d0265d06711645068" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23337/asset/image_n/jcc23337-fig-0001.png?v=1&amp;s=df389f1480edc5ac5b570e26aa9aa50c3c1471ff"/></a>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><!--Unmatched element: w:blockFixed--><p> Although phytochromes are a major family of photosensory proteins, there are fewer contributions to their characterization from computational modeling than for related photosensory proteins, which is likely because high-resolution structures of phytochromes are relatively scarce. Based on one such structure, Olle Falklöf and Bo Durbeej <!--TODO: clickthrough URL--><a href="http://dx.doi.org/10.1002/jcc.23265" title="Link to external resource: http://dx.doi.org/10.1002/jcc.23265">on page 1363</a> report hybrid quantum mechanics/molecular mechanics (QM/MM) calculations of UV-vis absorption spectra of a bacteriophytochrome. The calculations provide valuable information on how the choice of QM/MM methodology affects the resulting spectra, and they reveal how the protein tunes the absorption of its bilin chromophore relative to solvent and gas phase environments.</p></div>
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 Although phytochromes are a major family of photosensory proteins, there are fewer contributions to their characterization from computational modeling than for related photosensory proteins, which is likely because high-resolution structures of phytochromes are relatively scarce. Based on one such structure, Olle Falklöf and Bo Durbeej on page 1363 report hybrid quantum mechanics/molecular mechanics (QM/MM) calculations of UV-vis absorption spectra of a bacteriophytochrome. The calculations provide valuable information on how the choice of QM/MM methodology affects the resulting spectra, and they reveal how the protein tunes the absorption of its bilin chromophore relative to solvent and gas phase environments.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23265" xmlns="http://purl.org/rss/1.0/"><title>Modeling of phytochrome absorption spectra</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23265</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Modeling of phytochrome absorption spectra</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Olle Falklöf, Bo Durbeej</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-01T06:22:51.487308-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23265</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23265</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23265</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1363</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1374</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Phytochromes constitute one of the six well-characterized families of photosensory proteins in Nature. From the viewpoint of computational modeling, however, phytochromes have been the subject of much fewer studies than most other families of photosensory proteins, which is likely a consequence of relevant high-resolution structural data becoming available only in recent years. In this work, hybrid quantum mechanics/molecular mechanics (QM/MM) methods are used to calculate UV-vis absorption spectra of <em>Deinococcus radiodurans</em> bacteriophytochrome. We investigate how the choice of QM/MM methodology affects the resulting spectra and demonstrate that QM/MM methods can reproduce the experimental absorption maxima of both the Q and Soret bands with an accuracy of about 0.15 eV. Furthermore, we assess how the protein environment influences the intrinsic absorption of the bilin chromophore, with particular focus on the Q band underlying the primary photochemistry of phytochromes. © 2013 Wiley Periodicals, Inc.</p></div>
<a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/jcc.23265/asset/image_m/jcc23265-toc-0001-m.png?v=1&amp;s=87b5231a2b17adf96fd971a6409ed166a9eac028" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23265/asset/image_n/jcc23265-toc-0001.png?v=1&amp;s=96e8a11556d3e7a094ca1ff8e113c1b4e2dacd7a"/></a>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Hybrid quantum mechanics/molecular mechanics (QM/MM) methods are used to calculate UV-vis absorption spectra of a photosensory protein belonging to the phytochrome family. Besides providing valuable information on how the choice of QM/MM methodology affects the resulting spectra, the article also sheds new light on how the protein tunes the absorption of its bilin chromophore. </p><!--Unmatched element: w:blockFixed--></div>
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Phytochromes constitute one of the six well-characterized families of photosensory proteins in Nature. From the viewpoint of computational modeling, however, phytochromes have been the subject of much fewer studies than most other families of photosensory proteins, which is likely a consequence of relevant high-resolution structural data becoming available only in recent years. In this work, hybrid quantum mechanics/molecular mechanics (QM/MM) methods are used to calculate UV-vis absorption spectra of Deinococcus radiodurans bacteriophytochrome. We investigate how the choice of QM/MM methodology affects the resulting spectra and demonstrate that QM/MM methods can reproduce the experimental absorption maxima of both the Q and Soret bands with an accuracy of about 0.15 eV. Furthermore, we assess how the protein environment influences the intrinsic absorption of the bilin chromophore, with particular focus on the Q band underlying the primary photochemistry of phytochromes. © 2013 Wiley Periodicals, Inc.
Hybrid quantum mechanics/molecular mechanics (QM/MM) methods are used to calculate UV-vis absorption spectra of a photosensory protein belonging to the phytochrome family. Besides providing valuable information on how the choice of QM/MM methodology affects the resulting spectra, the article also sheds new light on how the protein tunes the absorption of its bilin chromophore. 




</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23267" xmlns="http://purl.org/rss/1.0/"><title>On-the-fly reconstruction of free-energy profiles using logarithmic mean-force dynamics</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23267</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">On-the-fly reconstruction of free-energy profiles using logarithmic mean-force dynamics</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Tetsuya Morishita, Satoru G. Itoh, Hisashi Okumura, Masuhiro Mikami</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-05T00:44:52.740409-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23267</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23267</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23267</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1375</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1384</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Mean-force dynamics (MFD), which is a fictitious dynamics for a set of collective variables on a potential of mean-force, is a powerful algorithm to efficiently explore free-energy landscapes. Recently, we have introduced logarithmic MFD (LogMFD) (Morishita et al., Phys. Rev. E 2012, 85, 066702) which overcomes difficulties encounterd in free-energy calculations using standard approaches such as thermodynamic integration. Here, we present a guide to implementing LogMFD calculations paying attention to the practical issues in choosing the parameters in LogMFD. A primary focus is given to the effect of the parameters on the accuracy of the reconstructed free-energy profiles. A recipe for reducing the errors due to energy dissipation is presented. We also demonstrate that multidimensional free-energy landscapes can be reconstructed on-the-fly using LogMFD, which cannot be accomplished using any other free-energy calculation techniques. © 2013 Wiley Periodicals, Inc.</p></div>
<a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/jcc.23267/asset/image_m/jcc23267-toc-0001-m.png?v=1&amp;s=4a87275e4ca6fd5f6909486b4b6f78247409f7a2" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23267/asset/image_n/jcc23267-toc-0001.png?v=1&amp;s=9cf9ab1c47289114d8a79f9429ac1c428aa702bd"/></a>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Logarithmic mean-force dynamics (LogMFD) is a method for free-energy calculation, which uses a logarithmic form of free energy to efficiently explore free-energy landscapes. Using LogMFD, one can obtain free-energy profiles on-the-fly without postprocessing. Here, we present a guide to using LogMFD detailing practical issues concerning the protocol for choosing the parameters and reducing errors due to energy dissipation. </p><!--Unmatched element: w:blockFixed--></div>
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Mean-force dynamics (MFD), which is a fictitious dynamics for a set of collective variables on a potential of mean-force, is a powerful algorithm to efficiently explore free-energy landscapes. Recently, we have introduced logarithmic MFD (LogMFD) (Morishita et al., Phys. Rev. E 2012, 85, 066702) which overcomes difficulties encounterd in free-energy calculations using standard approaches such as thermodynamic integration. Here, we present a guide to implementing LogMFD calculations paying attention to the practical issues in choosing the parameters in LogMFD. A primary focus is given to the effect of the parameters on the accuracy of the reconstructed free-energy profiles. A recipe for reducing the errors due to energy dissipation is presented. We also demonstrate that multidimensional free-energy landscapes can be reconstructed on-the-fly using LogMFD, which cannot be accomplished using any other free-energy calculation techniques. © 2013 Wiley Periodicals, Inc.
Logarithmic mean-force dynamics (LogMFD) is a method for free-energy calculation, which uses a logarithmic form of free energy to efficiently explore free-energy landscapes. Using LogMFD, one can obtain free-energy profiles on-the-fly without postprocessing. Here, we present a guide to using LogMFD detailing practical issues concerning the protocol for choosing the parameters and reducing errors due to energy dissipation. 




</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23271" xmlns="http://purl.org/rss/1.0/"><title>Automated discovery of chemically reasonable elementary reaction steps</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23271</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Automated discovery of chemically reasonable elementary reaction steps</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Paul M. Zimmerman</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-18T07:21:51.644318-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23271</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23271</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23271</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1385</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1392</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Due to the significant human effort and chemical intuition required to locate chemical reaction pathways with quantum chemical modeling, only a small subspace of possible reactions is usually investigated for any given system. Herein, a systematic approach is proposed for locating reaction paths that bypasses the required human effort and expands the reactive search space, all while maintaining low computational cost. To achieve this, a range of intermediates are generated that represent potential single elementary steps away from a starting structure. These structures are then screened to identify those that are thermodynamically accessible, and then feasible reaction paths to the remaining structures are located. This strategy for elementary reaction path finding is independent of atomistic model whenever bond breaking and forming are properly described. The approach is demonstrated to work well for upper main group elements, but this limitation can easily be surpassed. Further extension will allow discovery of multistep reaction mechanisms in a single computation. The method is highly parallel, allowing for effective use of modern large-scale computational clusters. © 2013 Wiley Periodicals, Inc.</p></div>
<a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/jcc.23271/asset/image_m/jcc23271-toc-0001-m.png?v=1&amp;s=75b0fc1de12b83f2694c1c2f629bb12546837999" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23271/asset/image_n/jcc23271-toc-0001.png?v=1&amp;s=611bf14bf7baa42eac24c0c8f1e56eed6a79bef3"/></a>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>A new method is proposed to find low barrier transition states starting from a single reactant complex. It operates by first generating chemically feasible structures and then uses a double-ended string method to locate reaction paths. The method in its current implementation should be highly useful for main group chemistry. </p><!--Unmatched element: w:blockFixed--></div>
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Due to the significant human effort and chemical intuition required to locate chemical reaction pathways with quantum chemical modeling, only a small subspace of possible reactions is usually investigated for any given system. Herein, a systematic approach is proposed for locating reaction paths that bypasses the required human effort and expands the reactive search space, all while maintaining low computational cost. To achieve this, a range of intermediates are generated that represent potential single elementary steps away from a starting structure. These structures are then screened to identify those that are thermodynamically accessible, and then feasible reaction paths to the remaining structures are located. This strategy for elementary reaction path finding is independent of atomistic model whenever bond breaking and forming are properly described. The approach is demonstrated to work well for upper main group elements, but this limitation can easily be surpassed. Further extension will allow discovery of multistep reaction mechanisms in a single computation. The method is highly parallel, allowing for effective use of modern large-scale computational clusters. © 2013 Wiley Periodicals, Inc.
A new method is proposed to find low barrier transition states starting from a single reactant complex. It operates by first generating chemically feasible structures and then uses a double-ended string method to locate reaction paths. The method in its current implementation should be highly useful for main group chemistry. 




</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23273" xmlns="http://purl.org/rss/1.0/"><title>Multireference calculations for ring inversion and double bond shifting in cyclooctatetraene</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23273</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Multireference calculations for ring inversion and double bond shifting in cyclooctatetraene</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Axel Schild, Beate Paulus</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-18T07:22:08.462245-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23273</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23273</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23273</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1393</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1397</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>We present multireference calculations for the characterization of ring inversion and double bond shifting in cyclooctatetraene. The results show that it is necessary to treat the dynamical correlation very accurately to obtain correct values for the barrier heights. This can be done, for example, with multireference configuration interaction or with perturbation theory of third order. However, detailed analysis also shows that already a complete active space self-consistent field treatment describes the processes surprisingly well. Thus, this method could be used as a computationally cheap method, for example, for dynamics simulations. © 2013 Wiley Periodicals, Inc.</p></div>
<a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/jcc.23273/asset/image_m/jcc23273-toc-0001-m.png?v=1&amp;s=405d53a67817e8d18bfd83ef984603d9465fed8a" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23273/asset/image_n/jcc23273-toc-0001.png?v=1&amp;s=a98f40a5def396ba8c8c5787ccabd43794df6763"/></a>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>In its electronic ground state, ring inversion and double bond shifting occur in cyclooctatetraene, as shown schematically in the picture. We use multireference calculation methods to determine the relevant structures of the ground-state potential energy surface for these processes. We also investigate at which level the dynamical and static electron correlations have to be treated to allow faithful numerical results. </p><!--Unmatched element: w:blockFixed--></div>
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We present multireference calculations for the characterization of ring inversion and double bond shifting in cyclooctatetraene. The results show that it is necessary to treat the dynamical correlation very accurately to obtain correct values for the barrier heights. This can be done, for example, with multireference configuration interaction or with perturbation theory of third order. However, detailed analysis also shows that already a complete active space self-consistent field treatment describes the processes surprisingly well. Thus, this method could be used as a computationally cheap method, for example, for dynamics simulations. © 2013 Wiley Periodicals, Inc.
In its electronic ground state, ring inversion and double bond shifting occur in cyclooctatetraene, as shown schematically in the picture. We use multireference calculation methods to determine the relevant structures of the ground-state potential energy surface for these processes. We also investigate at which level the dynamical and static electron correlations have to be treated to allow faithful numerical results. 




</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23276" xmlns="http://purl.org/rss/1.0/"><title>Free-energy differences between states with different conformational ensembles</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23276</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Free-energy differences between states with different conformational ensembles</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Jose Antonio Garate, Chris Oostenbrink</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-23T03:54:00.188468-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23276</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23276</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23276</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1398</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1408</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Multiple conformations separated by high-energy barriers represent a challenging problem in free-energy calculations due to the difficulties in achieving adequate sampling. We present an application of thermodynamic integration (TI) in conjunction with the local elevation umbrella sampling (LE/US) method to improve convergence in alchemical free-energy calculations. TI-LE/US was applied to the guanosine triphosphate (GTP) to 8-Br-GTP perturbation, molecules that present high-energy barriers between the anti and syn states and that have inverted preferences for those states. The convergence and reliability of TI-LE/US was assessed by comparing with previous results using the enhanced-sampling one-step perturbation (OSP) method. A linear interpolation of the end-state biasing potentials was sufficient to dramatically improve sampling along the chosen reaction coordinate. Conformational free-energy differences were also computed for the syn and anti states and compared to experimental and theoretical results. Additionally, a coupled OSP with LE/US was carried out, allowing the calculation of conformational and alchemical free energies of GTP and 8-substituted GTP analogs. © 2013 Wiley Periodicals, Inc.</p></div>
<a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/jcc.23276/asset/image_m/jcc23276-toc-0001-m.png?v=1&amp;s=e0b53520b0affea089b8a66693c80a4f64f2d789" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23276/asset/image_n/jcc23276-toc-0001.png?v=1&amp;s=7a8ba7bfd0eb4ea12d63e81b4cc4bcfebadbdc16"/></a>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Potential of mean force along the glycosidic χ angle (calculated using the LE/US method), at different λ points for the alchemical transformation GTP (λ = 0) to 8-Br-GTP (λ = 1). Note the shift in the population preference (syn–anti) during the progress of the alchemical transformation. </p><!--Unmatched element: w:blockFixed--></div>
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Multiple conformations separated by high-energy barriers represent a challenging problem in free-energy calculations due to the difficulties in achieving adequate sampling. We present an application of thermodynamic integration (TI) in conjunction with the local elevation umbrella sampling (LE/US) method to improve convergence in alchemical free-energy calculations. TI-LE/US was applied to the guanosine triphosphate (GTP) to 8-Br-GTP perturbation, molecules that present high-energy barriers between the anti and syn states and that have inverted preferences for those states. The convergence and reliability of TI-LE/US was assessed by comparing with previous results using the enhanced-sampling one-step perturbation (OSP) method. A linear interpolation of the end-state biasing potentials was sufficient to dramatically improve sampling along the chosen reaction coordinate. Conformational free-energy differences were also computed for the syn and anti states and compared to experimental and theoretical results. Additionally, a coupled OSP with LE/US was carried out, allowing the calculation of conformational and alchemical free energies of GTP and 8-substituted GTP analogs. © 2013 Wiley Periodicals, Inc.
Potential of mean force along the glycosidic χ angle (calculated using the LE/US method), at different λ points for the alchemical transformation GTP (λ = 0) to 8-Br-GTP (λ = 1). Note the shift in the population preference (syn–anti) during the progress of the alchemical transformation. 




</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23300" xmlns="http://purl.org/rss/1.0/"><title>Common vertex matrix: A novel characterization of molecular graphs by counting</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23300</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Common vertex matrix: A novel characterization of molecular graphs by counting</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Milan Randić, Marjana Novič, Dejan Plavšić</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-26T02:14:16.850973-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23300</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23300</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23300</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1409</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1419</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>We present a novel matrix representation of graphs based on the count of equal-distance common vertices to each pair of vertices in a graph. The element (<em>i</em>, <em>j</em>) of this matrix is defined as the number of vertices at the same distance from vertices (<em>i</em>, <em>j</em>). As illustrated on smaller alkanes, these novel matrices are very sensitive to molecular branching and the distribution of vertices in a graph. In particular, we show that ordered row sums of these novel matrices can facilitate solving graph isomorphism for acyclic graphs. This has been illustrated on all undecane isomers C<sub>11</sub>H<sub>24</sub> having the same path counts (total of 25 molecules), on pair of graphs on 18 vertices having the same distance degree sequences (Slater's graphs), as well as two graphs on 21 vertices having identical several topological indices derived from information on distances between vertices. © 2013 Wiley Periodicals, Inc.</p></div>
<a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/jcc.23300/asset/image_m/jcc23300-toc-0001-m.png?v=1&amp;s=53b0630d46ba5f4f983cbca903d9e1881dba1c44" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23300/asset/image_n/jcc23300-toc-0001.png?v=1&amp;s=b654090b7b884784955c9880663a2cfc73d85b39"/></a>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>We have outlined construction of a novel elementary matrix for graphs which may be of considerable interest for comparative study of molecules. The (<em>i</em>, <em>j</em>) matrix element of the novel matrix, referred to as the “Common Vertex Matrix,” is given by the count of vertices at equal distance from vertices <em>i</em> and <em>j</em>. Ordered row sums of the novel matrix (given as a sequence of integers) discriminates smaller acyclic molecular graphs quite well.
</p><!--Unmatched element: w:blockFixed--></div>
]]></content:encoded><description>
We present a novel matrix representation of graphs based on the count of equal-distance common vertices to each pair of vertices in a graph. The element (i, j) of this matrix is defined as the number of vertices at the same distance from vertices (i, j). As illustrated on smaller alkanes, these novel matrices are very sensitive to molecular branching and the distribution of vertices in a graph. In particular, we show that ordered row sums of these novel matrices can facilitate solving graph isomorphism for acyclic graphs. This has been illustrated on all undecane isomers C11H24 having the same path counts (total of 25 molecules), on pair of graphs on 18 vertices having the same distance degree sequences (Slater's graphs), as well as two graphs on 21 vertices having identical several topological indices derived from information on distances between vertices. © 2013 Wiley Periodicals, Inc.
We have outlined construction of a novel elementary matrix for graphs which may be of considerable interest for comparative study of molecules. The (i, j) matrix element of the novel matrix, referred to as the “Common Vertex Matrix,” is given by the count of vertices at equal distance from vertices i and j. Ordered row sums of the novel matrix (given as a sequence of integers) discriminates smaller acyclic molecular graphs quite well.






</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23272" xmlns="http://purl.org/rss/1.0/"><title>JACOB: An enterprise framework for computational chemistry</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23272</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">JACOB: An enterprise framework for computational chemistry</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Mark P. Waller, Thomas Dresselhaus, Jack Yang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-03T01:56:36.550494-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23272</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23272</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23272</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Software News and Updates</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1420</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1428</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Here, we present just a collection of beans (JACOB): an integrated batch-based framework designed for the rapid development of computational chemistry applications. The framework expedites developer productivity by handling the generic infrastructure tier, and can be easily extended by user-specific scientific code. Paradigms from enterprise software engineering were rigorously applied to create a scalable, testable, secure, and robust framework. A centralized web application is used to configure and control the operation of the framework. The application-programming interface provides a set of generic tools for processing large-scale noninteractive jobs (e.g., systematic studies), or for coordinating systems integration (e.g., complex workflows). The code for the JACOB framework is open sourced and is available at: <!--TODO: clickthrough URL--><a href="http://www.wallerlab.org/jacob" title="Link to external resource: http://www.wallerlab.org/jacob">www.wallerlab.org/jacob</a>. © 2013 Wiley Periodicals, Inc.</p></div>
<a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/jcc.23272/asset/image_m/jcc23272-toc-0001-m.png?v=1&amp;s=ae00b174b24077c887fadda3a2dd9cf4f13002d8" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23272/asset/image_n/jcc23272-toc-0001.png?v=1&amp;s=e32936c301fe3f7091c55ce5b265aa0e932e27f9"/></a>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>The implementation of an integrated framework for the future rapid development of computational chemistry applications is detailed. The multitiered infrastructure layer is based on enterprise programming paradigms. The code is available for download at <!--TODO: clickthrough URL--><a href="http://www.wallerlab.org" title="Link to external resource: http://www.wallerlab.org">www.wallerlab.org</a>. </p><!--Unmatched element: w:blockFixed--></div>
]]></content:encoded><description>
Here, we present just a collection of beans (JACOB): an integrated batch-based framework designed for the rapid development of computational chemistry applications. The framework expedites developer productivity by handling the generic infrastructure tier, and can be easily extended by user-specific scientific code. Paradigms from enterprise software engineering were rigorously applied to create a scalable, testable, secure, and robust framework. A centralized web application is used to configure and control the operation of the framework. The application-programming interface provides a set of generic tools for processing large-scale noninteractive jobs (e.g., systematic studies), or for coordinating systems integration (e.g., complex workflows). The code for the JACOB framework is open sourced and is available at: www.wallerlab.org/jacob. © 2013 Wiley Periodicals, Inc.
The implementation of an integrated framework for the future rapid development of computational chemistry applications is detailed. The multitiered infrastructure layer is based on enterprise programming paradigms. The code is available for download at www.wallerlab.org. 




</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23266" xmlns="http://purl.org/rss/1.0/"><title>NBO 6.0: Natural bond orbital analysis program</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23266</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">NBO 6.0: Natural bond orbital analysis program</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Eric D. Glendening, Clark R. Landis, Frank Weinhold</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-09T05:41:34.47297-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/jcc.23266</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/jcc.23266</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fjcc.23266</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Software News and Updates</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1429</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1437</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>We describe principal features of the newly released version, <em>NBO 6.0</em>, of the natural bond orbital analysis program, that provides novel “link-free” interactivity with host electronic structure systems, improved search algorithms and labeling conventions for a broader range of chemical species, and new analysis options that significantly extend the range of chemical applications. We sketch the motivation and implementation of program changes and describe newer analysis options with illustrative applications. © 2013 Wiley Periodicals, Inc.</p></div>
<a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/jcc.23266/asset/image_m/jcc23266-toc-0001-m.png?v=1&amp;s=412aebfbe6ab3050f2372a5fda2eee2a313b7b42" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/jcc.23266/asset/image_n/jcc23266-toc-0001.png?v=1&amp;s=11c5d870da1c8f8a1779ded45ab830684c499e31"/></a>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>A new version (NBO 6.0) of the natural bond orbital program significantly expands the range of chemical applications through a new link-free interface to host electronic structure systems, refined search algorithms, improved output labeling for exotic bonding motifs, and broadened range of analysis options. </p><!--Unmatched element: w:blockFixed--></div>
]]></content:encoded><description>
We describe principal features of the newly released version, NBO 6.0, of the natural bond orbital analysis program, that provides novel “link-free” interactivity with host electronic structure systems, improved search algorithms and labeling conventions for a broader range of chemical species, and new analysis options that significantly extend the range of chemical applications. We sketch the motivation and implementation of program changes and describe newer analysis options with illustrative applications. © 2013 Wiley Periodicals, Inc.
A new version (NBO 6.0) of the natural bond orbital program significantly expands the range of chemical applications through a new link-free interface to host electronic structure systems, refined search algorithms, improved output labeling for exotic bonding motifs, and broadened range of analysis options. 




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