| Autor: |
Aucar IA; Instituto de Modelado e Innovación Tecnológica, CONICET, and Departamento de Física - Facultad de Ciencias Exactas y Naturales, UNNE, Avda Libertad 5460, W3404AAS, Corrientes, Argentina. gaaucar@conicet.gov.ar., Gomez SS; Instituto de Modelado e Innovación Tecnológica, CONICET, and Departamento de Física - Facultad de Ciencias Exactas y Naturales, UNNE, Avda Libertad 5460, W3404AAS, Corrientes, Argentina. gaaucar@conicet.gov.ar., Giribet CG; Instituto de Física de Buenos Aires, CONICET, and Departamento de Física - Facultad de Ciencias Exactas y Naturales, UBA, Intendente Güiraldes 2160, Ciudad Universitaria, C1428EGA, Buenos Aires, Argentina., Aucar GA; Instituto de Modelado e Innovación Tecnológica, CONICET, and Departamento de Física - Facultad de Ciencias Exactas y Naturales, UNNE, Avda Libertad 5460, W3404AAS, Corrientes, Argentina. gaaucar@conicet.gov.ar. |
| Abstrakt: |
One of the most influential articles showing the best way to get the absolute values of NMR magnetic shieldings, σ (non-measurables) from both accurate measurements and theoretical calculations, was published a long time ago by Flygare. His model was shown to break down when heavy atoms are involved. This fact motivated the development of new theories of nuclear spin-rotation (SR) tensors, which consider electronic relativistic effects. One was published recently by some of us. In this article we take another step further and propose three different models that generalize Flygare's model. All of them are written using four-component relativistic expressions, though the two-component relativistic SO-S term also appears in one. The first clues for these developments were built from the relationship among σ and the SR tensors within the two-component relativistic LRESC model. Besides, we had to introduce a few other well defined assumptions: (i) relativistic corrections must be included in a way to best reproduce the relationship among the (e-e) term (called "paramagnetic" within the non-relativistic domain) of σ and its equivalent part of the SR tensor, (ii) as happens in Flygare's rule, the shielding of free atoms shall be included to improve accuracy. In the highest accurate model, a new term known as Spin-orbit due to spin, SO-S (in this mechanism the spin-Zeeman Hamiltonian replaces the orbital-Zeeman Hamiltonian), is included. We show the results of the application of those models to halogen containing linear molecules. |
