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Four-component Hartree-Fock calculations of magnetic-field induced circular birefringence-Faraday effect-in noble gases and dihalogens (Articolo in rivista)
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- Label
- Four-component Hartree-Fock calculations of magnetic-field induced circular birefringence-Faraday effect-in noble gases and dihalogens (Articolo in rivista) (literal)
- Anno
- 2005-01-01T00:00:00+01:00 (literal)
- Alternative label
Ekstroem, U.; Norman, P.; Rizzo, A. (2005)
Four-component Hartree-Fock calculations of magnetic-field induced circular birefringence-Faraday effect-in noble gases and dihalogens
(literal)
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- Ekstroem, U.; Norman, P.; Rizzo, A. (literal)
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- ISI Web of Science (WOS) (literal)
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- Department of Physics and Measurement Technology, Linköping University, SE-581 83 Linköping, Sweden
Istituto per i Processi Chimico-Fisici, Consiglio Nazionale delle Ricerche, Area della Ricerca,
via G. Moruzzi 1, loc. S. Cataldo, I-56124 Pisa, Italy (literal)
- Titolo
- Four-component Hartree-Fock calculations of magnetic-field induced circular birefringence-Faraday effect-in noble gases and dihalogens (literal)
- Abstract
- The effects of relativity on the magnetic-field induced circular birefringence, or Faraday effect, in
He, Ne, Ar, Xe, Rn, F2, Cl2, Br2, and I2 have been determined at the four-component HartreeFock
level of theory. A measure of the birefringence is given by the Verdet constant, which is a third-order
molecular property and thus relates to quadratic response functions. A fully analytical nonlinear
polarization propagator approach is employed. The results are gauge invariant as a consequence of
the spatial symmetries in the molecular systems. The calculations include electronic as well as
vibrational contributions to the property. Comparison with experiment is made for He, Ne, Ar, Xe,
and Cl2, and, apart from neon, the theoretical values of the Verdet constant are within 10% of the
experimental ones. The inclusion of nonrelativistically spin-forbidden excitations in the propagator
parametrization has significant effects on the dispersion in general, but such effects are in the
general case largely explained by the use of a resonant-divergent propagator theory. In the present
work we do, however, observe noticeable relativistic corrections to the Verdet constant in the
off-resonant regions for systems with light elements (F2 and Cl2), and nonrelativistic results for the
Verdet constant of Br2 are in error by 25% in the low-frequency region. (literal)
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