Chapter 15. External Electromagnetic Fields and Molecular Properties
Published Online: 22 JUN 2009
DOI: 10.1002/9783527627486.ch15
Copyright © 2009 Wiley-VCH Verlag GmbH & Co. KGaA
Book Title

Relativistic Quantum Chemistry: The Fundamental Theory of Molecular Science
Additional Information
How to Cite
Reiher, M. and Wolf, A. (2009) External Electromagnetic Fields and Molecular Properties, in Relativistic Quantum Chemistry: The Fundamental Theory of Molecular Science, Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim, Germany. doi: 10.1002/9783527627486.ch15
Publication History
- Published Online: 22 JUN 2009
- Published Print: 14 JAN 2009
ISBN Information
Print ISBN: 9783527312924
Online ISBN: 9783527627486
- Summary
- Chapter
Keywords:
- external electromagnetic fields;
- molecular properties;
- four-component perturbation;
- response theory;
- two-component form;
- picture change artifacts;
- Douglas–Kroll–Hess property transformation;
- magnetic fields in resonance spectroscopies;
- electric field gradient;
- nuclear quadrupole moment;
- parity violation;
- electro-weak chemistry
Summary
The relativistic calculation of observables and molecular properties follows the lines elaborated first in nonrelativistic quantum chemistry, in which the small electromagnetic perturbation is considered in a Taylor expansion of the electronic energy. Molecular properties are then defined as the derivatives in this expansion. However, the relativistic minimal coupling principle allows for a rigorous inclusion of electromagnetic fields. Thus, four-component theory of response properties derived from this perturbation is naturally a consistent framework. Such a theory, however, requires the perturbed wave function, which is usually expanded in terms of the set of eigenfunctions of the unperturbed Hamiltonian so that the role of the negative-energy states has to be clarified. In particular, they become decisive for the explanation of the diamagnetic contribution of magnetic-response parameters. Again, two-component schemes are free of negative-energy states, but this benefit needs to be analyzed carefully. Also, they suffer from the so-called picture-change error.
