<?xml version="1.0" encoding="UTF-8"?>
<rdf:RDF xmlns:rdf="http://www.w3.org/1999/02/22-rdf-syntax-ns#"><channel rdf:about="http://onlinelibrary.wiley.com/rss/journal/10.1002/(ISSN)1612-202X" xmlns="http://purl.org/rss/1.0/"><title>Laser Physics Letters</title><description> Wiley Online Library : Laser Physics Letters</description><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2F%28ISSN%291612-202X</link><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc</dc:publisher><dc:language xmlns:dc="http://purl.org/dc/elements/1.1/">en</dc:language><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/">Copyright © 2013 WILEY-VCH Verlag GmbH &amp; Co. KGaA, Weinheim</dc:rights><prism:issn xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1612-2011</prism:issn><prism:eIssn xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1612-202X</prism:eIssn><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-04-01T00:00:00-05:00</dc:date><prism:coverDisplayDate xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">April 2012</prism:coverDisplayDate><prism:volume xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">9</prism:volume><prism:number xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">4</prism:number><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">253</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">328</prism:endingPage><image rdf:resource="http://onlinelibrary.wiley.com/store/10.1002/lapl.v9.4/asset/cover.gif?v=1&amp;s=b7bf846c9cd0f1480f3fe1610c77fabfc1de2132"/><items><rdf:Seq><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201290006"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201290008"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201290007"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201110102"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201110121"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201110128"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201110133"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201110136"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201110135"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201110132"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201110126"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201110134"/></rdf:Seq></items></channel><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201290006" xmlns="http://purl.org/rss/1.0/"><title>Cover Picture: Laser Phys. Lett. 4/2012</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201290006</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Cover Picture: Laser Phys. Lett. 4/2012</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-03-14T03:22:16.515617-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/lapl.201290006</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/lapl.201290006</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201290006</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Cover Picture</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>Example of a color image (taken with a hand-held CCD-photocamera Samsung WB 500) of the spatially distributed conical components of parametric multi-wavelength anti-Stokes RFWM lasing (“anti-Stokes laser rainbow”) of an aragonite single crystal recorded at room temperature under picosecond pumping at <em>λ</em><sub><em>f</em>1</sub> = 1.06415 µm wavelength in excitation geometry <b>e</b><sub>3</sub>[<b>e</b><sub>1</sub><b>e</b><sub>1</sub>]<b>e</b><sub>3</sub> (Cover picture: A.A. Kaminskii, H. Rhee, et al. pp. 259–284, in this issue) (© 2011 by Astro Ltd., Published exclusively by WILEY-VCH Verlag GmbH &amp; Co. KGaA)</p></div>]]></content:encoded><description>Example of a color image (taken with a hand-held CCD-photocamera Samsung WB 500) of the spatially distributed conical components of parametric multi-wavelength anti-Stokes RFWM lasing (“anti-Stokes laser rainbow”) of an aragonite single crystal recorded at room temperature under picosecond pumping at λf1 = 1.06415 µm wavelength in excitation geometry e3[e1e1]e3 (Cover picture: A.A. Kaminskii, H. Rhee, et al. pp. 259–284, in this issue) (© 2011 by Astro Ltd., Published exclusively by WILEY-VCH Verlag GmbH &amp; Co. KGaA)</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201290008" xmlns="http://purl.org/rss/1.0/"><title>Issue Information: Laser Phys. Lett. /2012</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201290008</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Issue Information: Laser Phys. Lett. /2012</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-03-14T03:22:16.515617-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/lapl.201290008</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/lapl.201290008</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201290008</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Issue Information</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%2Flapl.201290007" xmlns="http://purl.org/rss/1.0/"><title>Contents: Laser Phys. Lett. 4/2012</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201290007</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Contents: Laser Phys. Lett. 4/2012</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-03-14T03:22:16.515617-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/lapl.201290007</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/lapl.201290007</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201290007</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Contents</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">253</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">258</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%2Flapl.201110102" xmlns="http://purl.org/rss/1.0/"><title>Stimulated Raman scattering spectroscopy and χ(3)-nonlinear lasing effects in single crystals of aragonite (orthorhombic CaCO3)</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201110102</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Stimulated Raman scattering spectroscopy and χ(3)-nonlinear lasing effects in single crystals of aragonite (orthorhombic CaCO3)</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">A.A. Kaminskii, H. Rhee, O. Lux, H.J. Eichler, V.V. Koltashev, R. Kleinschrodt, L. Bohatý, P. Becker</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-01-30T08:10:22.295993-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/lapl.201110102</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/lapl.201110102</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201110102</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Brief Reviews Invited Articles</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">259</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">284</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 present work gives a brief review of the nonlinear <em>χ</em><sup>(2)</sup>- and <em>χ</em><sup>(3)</sup>-lasing properties of SRS-active natural crystals (minerals) known so far. This compilation complements new results of a detailed investigation of Raman induced <em>χ</em><sup>(3)</sup>-effects in aragonite single crystals (orthorhombic CaCO<sub>3</sub>) under single- and dual-wavelength picosecond excitation in the UV, visible and near-IR spectral ranges. The studied effects at room and cryogenic temperatures comprise Stokes and anti-Stokes combs of almost two octaves bandwidth, THG, SFG, as well as cascaded and cross-cascaded <em>χ</em><sup>(3)</sup> ↔ <em>χ</em><sup>(3)</sup> interactions. All recorded lasing <em>χ</em><sup>(3)</sup>-components were identified and attributed to three observed SRS-promoting vibration modes <em>ω</em><sub><em>SRS</em> 1</sub> ≈ 1087 cm<sup>–1</sup>, <em>ω</em><sub><em>SRS</em> 2</sub> ≈ 152 cm<sup>–1</sup>, and <em>ω</em><sub><em>SRS</em> 3</sub> ≈ 205 cm<sup>–1</sup> (at room temperature) of aragonite. Stimulated Raman scattering (SRS) investigations of minerals so far enrich the arsenal of SRS-active crystals, which can be applied to solve fundamental and applied tasks of modern laser physics and nonlinear optics. (© 2012 by Astro Ltd., Published exclusively by WILEY-VCH Verlag GmbH &amp; Co. KGaA) (© 2011 by Astro Ltd., Published exclusively by WILEY-VCH Verlag GmbH &amp; Co. KGaA)</p></div>]]></content:encoded><description>The present work gives a brief review of the nonlinear χ(2)- and χ(3)-lasing properties of SRS-active natural crystals (minerals) known so far. This compilation complements new results of a detailed investigation of Raman induced χ(3)-effects in aragonite single crystals (orthorhombic CaCO3) under single- and dual-wavelength picosecond excitation in the UV, visible and near-IR spectral ranges. The studied effects at room and cryogenic temperatures comprise Stokes and anti-Stokes combs of almost two octaves bandwidth, THG, SFG, as well as cascaded and cross-cascaded χ(3) ↔ χ(3) interactions. All recorded lasing χ(3)-components were identified and attributed to three observed SRS-promoting vibration modes ωSRS 1 ≈ 1087 cm–1, ωSRS 2 ≈ 152 cm–1, and ωSRS 3 ≈ 205 cm–1 (at room temperature) of aragonite. Stimulated Raman scattering (SRS) investigations of minerals so far enrich the arsenal of SRS-active crystals, which can be applied to solve fundamental and applied tasks of modern laser physics and nonlinear optics. (© 2012 by Astro Ltd., Published exclusively by WILEY-VCH Verlag GmbH &amp; Co. KGaA) (© 2011 by Astro Ltd., Published exclusively by WILEY-VCH Verlag GmbH &amp; Co. KGaA)</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201110121" xmlns="http://purl.org/rss/1.0/"><title>Spectroscopic properties and laser performance of a new mixed Yb0.015:Lu0.162Gd0.823VO4 crystal</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201110121</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Spectroscopic properties and laser performance of a new mixed Yb0.015:Lu0.162Gd0.823VO4 crystal</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">J. Liu, W. Kong, W. Han, H. Zhang, X. Mateos, V. Petrov</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-01-30T08:10:26.284406-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/lapl.201110121</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/lapl.201110121</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201110121</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Solid State and Liquid Lasers</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">285</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">290</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>Spectroscopic properties and continuous-wave laser performance of a new Yb<sub>0.015</sub>:Lu<sub>0.162</sub>Gd<sub>0.823</sub>VO<sub>4</sub> mixed vanadate crystal are reported. An appreciable discontinuous increase in output power occurs during the <em>σ</em> - to <em>π</em> -polarization switching process in the laser oscillation. A maximum output power of 4.3 W is generated with an optical-to-optical efficiency of 46%, whereas the average slope efficiency is determined to be 73–77%, depending on the output coupling utilized. (© 2012 by Astro Ltd., Published exclusively by WILEY-VCH Verlag GmbH &amp; Co. KGaA) (© 2011 by Astro Ltd., Published exclusively by WILEY-VCH Verlag GmbH &amp; Co. KGaA)</p></div>]]></content:encoded><description>Spectroscopic properties and continuous-wave laser performance of a new Yb0.015:Lu0.162Gd0.823VO4 mixed vanadate crystal are reported. An appreciable discontinuous increase in output power occurs during the σ - to π -polarization switching process in the laser oscillation. A maximum output power of 4.3 W is generated with an optical-to-optical efficiency of 46%, whereas the average slope efficiency is determined to be 73–77%, depending on the output coupling utilized. (© 2012 by Astro Ltd., Published exclusively by WILEY-VCH Verlag GmbH &amp; Co. KGaA) (© 2011 by Astro Ltd., Published exclusively by WILEY-VCH Verlag GmbH &amp; Co. KGaA)</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201110128" xmlns="http://purl.org/rss/1.0/"><title>Compact passively Q-switched diode-pumped Tm:KY(WO4)2 laser with 8 ns/30/LJ pulses</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201110128</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Compact passively Q-switched diode-pumped Tm:KY(WO4)2 laser with 8 ns/30/LJ pulses</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">M.S. Gaponenko, A.A. Onushchenko, V.E. Kisel, A.M. Malyarevich, K.V. Yumashev, N.V. Kuleshov</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-01-30T08:10:29.40397-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/lapl.201110128</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/lapl.201110128</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201110128</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">291</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">294</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>A compact diode-pumped solid-state Tm:KY(WO<sub>4</sub>)<sub>2</sub> laser with cavity length of 1 cm passively Q-switched with a PbS-quantum-dot-based saturable absorber is presented. The laser operates at the wavelength of 1.94 µm and produces pulses with duration of 8 ns and energy of 30 µJ at the repetition rate up to 4.2 kHz. The maximum output power of 120 mW is achieved at incident pump power of 1.15 W. (© 2012 by Astro Ltd., Published exclusively by WILEY-VCH Verlag GmbH &amp; Co. KGaA) (© 2011 by Astro Ltd., Published exclusively by WILEY-VCH Verlag GmbH &amp; Co. KGaA)</p></div>]]></content:encoded><description>A compact diode-pumped solid-state Tm:KY(WO4)2 laser with cavity length of 1 cm passively Q-switched with a PbS-quantum-dot-based saturable absorber is presented. The laser operates at the wavelength of 1.94 µm and produces pulses with duration of 8 ns and energy of 30 µJ at the repetition rate up to 4.2 kHz. The maximum output power of 120 mW is achieved at incident pump power of 1.15 W. (© 2012 by Astro Ltd., Published exclusively by WILEY-VCH Verlag GmbH &amp; Co. KGaA) (© 2011 by Astro Ltd., Published exclusively by WILEY-VCH Verlag GmbH &amp; Co. KGaA)</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201110133" xmlns="http://purl.org/rss/1.0/"><title>Diode-pumped continuous-wave blue laser operation of Nd:GGG at 467.0, 467.7, and 468.5 nm</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201110133</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Diode-pumped continuous-wave blue laser operation of Nd:GGG at 467.0, 467.7, and 468.5 nm</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">B. Xu, P. Camy, J.L. Doualan, A. Braud, Z.P. Cai, A. Brenier, R. Moncorgé</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-01-30T08:10:35.138833-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/lapl.201110133</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/lapl.201110133</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201110133</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">295</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">300</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>Intra-cavity frequency doubling of continuous-wave (CW) laser emission on the quasi-three level (<sup>4</sup>F<sub>3/2</sub> → <sup>4</sup>I<sub>9/2</sub>) laser transition of Nd<sup>3+</sup> in Nd:GGG is reported by using a three-mirror folded resonator. The thermal lens experienced by the optically-pumped Nd:GGG laser crystal is measured as a function of the absorbed pump power and compared to that found, in the same conditions, in the case of Nd:YAG. Results are interpreted by using a simple model accounting for the absorbed pump power and the thermo-mechanical properties of each laser crystal. Diode-pumped blue laser operation is achieved, for the first time, at 467.0 and 468.5 nm with output powers of 230 and 450 mW, respectively. Simultaneous laser operation resulting both from frequency-doubling and frequency summing at the three 467.1, 467.7, and 468.1 nm laser wavelengths is also obtained with a total output power of 60 mW. (© 2012 by Astro Ltd., Published exclusively by WILEY-VCH Verlag GmbH &amp; Co. KGaA) (© 2011 by Astro Ltd., Published exclusively by WILEY-VCH Verlag GmbH &amp; Co. KGaA)</p></div>]]></content:encoded><description>Intra-cavity frequency doubling of continuous-wave (CW) laser emission on the quasi-three level (4F3/2 → 4I9/2) laser transition of Nd3+ in Nd:GGG is reported by using a three-mirror folded resonator. The thermal lens experienced by the optically-pumped Nd:GGG laser crystal is measured as a function of the absorbed pump power and compared to that found, in the same conditions, in the case of Nd:YAG. Results are interpreted by using a simple model accounting for the absorbed pump power and the thermo-mechanical properties of each laser crystal. Diode-pumped blue laser operation is achieved, for the first time, at 467.0 and 468.5 nm with output powers of 230 and 450 mW, respectively. Simultaneous laser operation resulting both from frequency-doubling and frequency summing at the three 467.1, 467.7, and 468.1 nm laser wavelengths is also obtained with a total output power of 60 mW. (© 2012 by Astro Ltd., Published exclusively by WILEY-VCH Verlag GmbH &amp; Co. KGaA) (© 2011 by Astro Ltd., Published exclusively by WILEY-VCH Verlag GmbH &amp; Co. KGaA)</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201110136" xmlns="http://purl.org/rss/1.0/"><title>Laser properties of Fe:Cr:Zn1–xMgxSe crystal for tunable mid-infrared laser sources</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201110136</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Laser properties of Fe:Cr:Zn1–xMgxSe crystal for tunable mid-infrared laser sources</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">M.E. Doroshenko, H. Jelínková, J. Šulc, M. Jelínek, M. Němec, T.T. Basiev, Y.A. Zagoruiko, N.O. Kovalenko, A.S. Gerasimenko, V.M. Puzikov</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-01-30T08:10:40.780234-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/lapl.201110136</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/lapl.201110136</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201110136</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">301</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">305</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 characterization of new gain-switched Fe:Cr:Zn<sub>1–<em>x</em></sub>Mg<sub><em>x</em></sub>Se laser working at the room temperature and its comparison to Fe:ZnSe laser was performed. The laser oscillation behavior, generation efficiency and output wavelength tuning possibilities were demonstrated. It was shown that the absorption and luminescence spectra of Fe:Cr:ZnMgSe crystal are shifted towards longer wavelengths in comparison with Fe:ZnSe active material. The difference is approximately 300 nm and it corresponds to measured absorption and emission spectra. The maximal Fe:Cr:ZnMgSe laser generated energy and the slope efficiency with respect to the absorbed energy were 200 µJ and 4.5%, respectively. (© 2012 by Astro Ltd., Published exclusively by WILEY-VCH Verlag GmbH &amp; Co. KGaA) (© 2011 by Astro Ltd., Published exclusively by WILEY-VCH Verlag GmbH &amp; Co. KGaA)</p></div>]]></content:encoded><description>The characterization of new gain-switched Fe:Cr:Zn1–xMgxSe laser working at the room temperature and its comparison to Fe:ZnSe laser was performed. The laser oscillation behavior, generation efficiency and output wavelength tuning possibilities were demonstrated. It was shown that the absorption and luminescence spectra of Fe:Cr:ZnMgSe crystal are shifted towards longer wavelengths in comparison with Fe:ZnSe active material. The difference is approximately 300 nm and it corresponds to measured absorption and emission spectra. The maximal Fe:Cr:ZnMgSe laser generated energy and the slope efficiency with respect to the absorbed energy were 200 µJ and 4.5%, respectively. (© 2012 by Astro Ltd., Published exclusively by WILEY-VCH Verlag GmbH &amp; Co. KGaA) (© 2011 by Astro Ltd., Published exclusively by WILEY-VCH Verlag GmbH &amp; Co. KGaA)</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201110135" xmlns="http://purl.org/rss/1.0/"><title>High-order stimulated Raman scattering in tetragonal CaYAlO4 crystal-host for Ln3+-lasant ions</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201110135</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">High-order stimulated Raman scattering in tetragonal CaYAlO4 crystal-host for Ln3+-lasant ions</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">A.A. Kaminskii, X. Xu, O. Lux, H. Rhee, H.J. Eichler, J. Zhang, D. Zhou, A. Shirakawa, K. Ueda, J. Xu</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-01-30T08:10:39.634873-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/lapl.201110135</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/lapl.201110135</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201110135</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Laser Spectroscopy</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">306</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">311</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>Multiple Stokes and anti-Stokes <em>χ</em><sup>(3)</sup>-nonlinear generation in the tetragonal crystal of CaYAlO<sub>4</sub> was observed at 300K and ≈9K under picosecond excitation in the visible spectral range. All the recorded Raman induced laser lines were identified and attributed to the SRS-promoting vibration mode of octahedral [AlO<sub>6</sub>]<sup>–9</sup> units of the crystal. (© 2012 by Astro Ltd., Published exclusively by WILEY-VCH Verlag GmbH &amp; Co. KGaA) (© 2011 by Astro Ltd., Published exclusively by WILEY-VCH Verlag GmbH &amp; Co. KGaA)</p></div>]]></content:encoded><description>Multiple Stokes and anti-Stokes χ(3)-nonlinear generation in the tetragonal crystal of CaYAlO4 was observed at 300K and ≈9K under picosecond excitation in the visible spectral range. All the recorded Raman induced laser lines were identified and attributed to the SRS-promoting vibration mode of octahedral [AlO6]–9 units of the crystal. (© 2012 by Astro Ltd., Published exclusively by WILEY-VCH Verlag GmbH &amp; Co. KGaA) (© 2011 by Astro Ltd., Published exclusively by WILEY-VCH Verlag GmbH &amp; Co. KGaA)</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201110132" xmlns="http://purl.org/rss/1.0/"><title>New modality in optical microscopy based on laser with injected radiation</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201110132</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">New modality in optical microscopy based on laser with injected radiation</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">S.A. Gonchukov, T.V. Lonkina, V.M. Yermachenko</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-01-30T08:10:30.997063-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/lapl.201110132</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/lapl.201110132</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201110132</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Interaction of Laser Radiation with Matter</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">312</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">316</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>In this work it is shown, that laser with injection of reflected radiation can possess the high longitudinal spatial selectivity. Laser figures here both the emitter and the detector of radiation. This attribute, having volumetric character for laser fields, can be considered as a new modality in optical microscopy. Using the experimental possibilities we achieved the spatial resolution at a level of several microns. The optimization of laser sources is to lead to longitudinal spatial resolution at a level of nanometers. (© 2012 by Astro Ltd., Published exclusively by WILEY-VCH Verlag GmbH &amp; Co. KGaA) (© 2011 by Astro Ltd., Published exclusively by WILEY-VCH Verlag GmbH &amp; Co. KGaA)</p></div>]]></content:encoded><description>In this work it is shown, that laser with injection of reflected radiation can possess the high longitudinal spatial selectivity. Laser figures here both the emitter and the detector of radiation. This attribute, having volumetric character for laser fields, can be considered as a new modality in optical microscopy. Using the experimental possibilities we achieved the spatial resolution at a level of several microns. The optimization of laser sources is to lead to longitudinal spatial resolution at a level of nanometers. (© 2012 by Astro Ltd., Published exclusively by WILEY-VCH Verlag GmbH &amp; Co. KGaA) (© 2011 by Astro Ltd., Published exclusively by WILEY-VCH Verlag GmbH &amp; Co. KGaA)</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201110126" xmlns="http://purl.org/rss/1.0/"><title>Transmission spectroscopy of dengue viral infection</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201110126</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Transmission spectroscopy of dengue viral infection</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">S. Firdous, M. Ahmed, A. Rehman, M. Nawaz, S. Anwar, S. Murtaza</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-01-30T08:10:27.594088-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/lapl.201110126</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/lapl.201110126</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201110126</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Laser Methods in Chemistry, Biology, and Medicine</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">317</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">321</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>We presented the rapid diagnostic test for dengue infection based on light spectrum of human blood. The transmission spectra of dengue infected whole blood samples have been recorded in ultra violet to near infrared range (400–800 nm) of about 30 conformed infected patients and compared to normal blood samples. Transmission spectra of dengue infected blood illustrate a strong band from 400–600 nm with prominant peaks at 540 and 580 nm, where is in case of normal blood below 600 nm, total absorption has been observed. These prominent peaks from 400–600 nm are characteristics of cells damage and dangue virus antibodies immunoglobulin G (IgG) and immunoglobulin M (IgM) produced against dengue antigen. The presented diagnostic method is non invasive, cost effective, easy and fast screening technique for dengue infected patients. (© 2012 by Astro Ltd., Published exclusively by WILEY-VCH Verlag GmbH &amp; Co. KGaA) (© 2011 by Astro Ltd., Published exclusively by WILEY-VCH Verlag GmbH &amp; Co. KGaA)</p></div>]]></content:encoded><description>We presented the rapid diagnostic test for dengue infection based on light spectrum of human blood. The transmission spectra of dengue infected whole blood samples have been recorded in ultra violet to near infrared range (400–800 nm) of about 30 conformed infected patients and compared to normal blood samples. Transmission spectra of dengue infected blood illustrate a strong band from 400–600 nm with prominant peaks at 540 and 580 nm, where is in case of normal blood below 600 nm, total absorption has been observed. These prominent peaks from 400–600 nm are characteristics of cells damage and dangue virus antibodies immunoglobulin G (IgG) and immunoglobulin M (IgM) produced against dengue antigen. The presented diagnostic method is non invasive, cost effective, easy and fast screening technique for dengue infected patients. (© 2012 by Astro Ltd., Published exclusively by WILEY-VCH Verlag GmbH &amp; Co. KGaA) (© 2011 by Astro Ltd., Published exclusively by WILEY-VCH Verlag GmbH &amp; Co. KGaA)</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201110134" xmlns="http://purl.org/rss/1.0/"><title>Accurate and noninvasive embryos screening during in vitro fertilization (IVF) assisted by Raman analysis ofembryos culture medium</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201110134</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Accurate and noninvasive embryos screening during in vitro fertilization (IVF) assisted by Raman analysis ofembryos culture medium</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">A.G. Shen, J. Peng, Q.H. Zhao, L. Su, X.H. Wang, J.M. Hu, Q. Yang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-01-30T08:10:38.273926-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/lapl.201110134</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/lapl.201110134</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Flapl.201110134</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Laser Methods in Chemistry, Biology, and Medicine</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">322</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">328</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>In combination with morphological evaluation tests, we employ Raman spectroscopy to select higher potential reproductive embryos during in vitro fertilization (IVF) based on chemical composition of embryos culture medium. In this study, 57 Raman spectra are acquired from both higher and lower quality embryos culture medium (ECM) from 10 patients which have been preliminarily confirmed by clinical assay. Data are fit by using a linear combination model of least squares method in which 12 basis spectra represent the chemical features of ECM. The final fitting coefficients provide insight into the chemical compositions of culture medium samples and are subsequently used as criterion to evaluate the quality of embryos. The relative fitting coefficients ratios of sodium pyruvate/albumin and phenylalanine/albumin seem act as key roles in the embryo screening, attaining 85.7% accuracy in comparison with clinical pregnancy. The good results demonstrate that Raman spectroscopy therefore is an important candidate for an accurate and noninvasive screening of higher quality embryos, which potentially decrease the time-consuming clinical trials during IVF. (© 2012 by Astro Ltd., Published exclusively by WILEY-VCH Verlag GmbH &amp; Co. KGaA) (© 2011 by Astro Ltd., Published exclusively by WILEY-VCH Verlag GmbH &amp; Co. KGaA)</p></div>]]></content:encoded><description>In combination with morphological evaluation tests, we employ Raman spectroscopy to select higher potential reproductive embryos during in vitro fertilization (IVF) based on chemical composition of embryos culture medium. In this study, 57 Raman spectra are acquired from both higher and lower quality embryos culture medium (ECM) from 10 patients which have been preliminarily confirmed by clinical assay. Data are fit by using a linear combination model of least squares method in which 12 basis spectra represent the chemical features of ECM. The final fitting coefficients provide insight into the chemical compositions of culture medium samples and are subsequently used as criterion to evaluate the quality of embryos. The relative fitting coefficients ratios of sodium pyruvate/albumin and phenylalanine/albumin seem act as key roles in the embryo screening, attaining 85.7% accuracy in comparison with clinical pregnancy. The good results demonstrate that Raman spectroscopy therefore is an important candidate for an accurate and noninvasive screening of higher quality embryos, which potentially decrease the time-consuming clinical trials during IVF. (© 2012 by Astro Ltd., Published exclusively by WILEY-VCH Verlag GmbH &amp; Co. KGaA) (© 2011 by Astro Ltd., Published exclusively by WILEY-VCH Verlag GmbH &amp; Co. KGaA)</description></item></rdf:RDF>