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Titlebook: Relativistic Effects in Atoms, Molecules, and Solids; G. L. Malli Book 1983 Plenum Press, New York 1983 atoms.cluster.electron.energy.mole

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41#
發(fā)表于 2025-3-28 17:35:19 | 只看該作者
Jaime Keller D.E.Pg.systems ?Random fractals ?Fractals and dynamical systems, and ?Harmonic analysis on fractals. The reader will be introduced to the most recent results in these subjects. Researchers and graduate students alike will benefit from the clear expositions.978-3-0348-7757-2978-3-0348-7755-8Series ISSN 1050-6977 Series E-ISSN 2297-0428
42#
發(fā)表于 2025-3-28 22:09:27 | 只看該作者
43#
發(fā)表于 2025-3-29 00:18:04 | 只看該作者
44#
發(fā)表于 2025-3-29 03:15:36 | 只看該作者
45#
發(fā)表于 2025-3-29 09:06:14 | 只看該作者
Self-Consistency and Numerical Problems, of Slater integrals involving only radial functions defined in terms of a suitable one-body potential. From this point on, the process is very close to that employed in non-relativistic calculations of similar type.
46#
發(fā)表于 2025-3-29 12:07:58 | 只看該作者
47#
發(fā)表于 2025-3-29 18:23:40 | 只看該作者
Lamb Shift in High-Z Atoms, instantaneous Coulomb interaction between electrons and nuclei. However, relativistic effects can play an important role in the quantitative description of such systems, as discussed in the accompanying papers in these proceedings. For a many-electron system, the relativistic description is formula
48#
發(fā)表于 2025-3-29 22:10:25 | 只看該作者
,Calculation of Relativistic Effects in Atoms and Molecules from the Schr?dinger Wave Function,amics and a many-electron generalization of the one-electron Dirac theory. On the whole, results calculated from this theory agree with experimental data. Nevertheless, the theory is by no means entirely satisfactory; in its development, certain ambiguities and divergencies are resolved by somewhat
49#
發(fā)表于 2025-3-29 23:58:55 | 只看該作者
50#
發(fā)表于 2025-3-30 07:50:58 | 只看該作者
Dirac-Fock One-Centre Expansion Method, the speed of light, i.e. the inner electrons of heavy atoms, but also for the valence electrons of medium and high Z atoms. The underlying reasons are first that the valence electrons themselves have an instantaneous velocity which becomes appreciable when they come close to the nucleus. Second we
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