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Titlebook: Quantum Mechanics; Foundations and Appl Arno Bohm Textbook 19862nd edition Springer Science+Business Media New York 1986 Cross section.Func

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51#
發(fā)表于 2025-3-30 08:16:52 | 只看該作者
52#
發(fā)表于 2025-3-30 13:38:48 | 只看該作者
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發(fā)表于 2025-3-30 17:19:34 | 只看該作者
54#
發(fā)表于 2025-3-30 22:38:11 | 只看該作者
,Addition of Angular Momenta—The Wigner-Eckart Theorem,V.2 discusses then the direct product of two irreducible representations of angular momentum and its reduction with respect to the total angular momentum. The Clebsch-Gordan coefficients are introduced, their recursion relations are derived, and their most frequently used values are tabulated. In Se
55#
發(fā)表于 2025-3-31 02:50:00 | 只看該作者
56#
發(fā)表于 2025-3-31 06:33:08 | 只看該作者
,Alkali Atoms and the Schr?dinger Equation of One-Electron Atoms,ion of the matrix elements of .. (. = 1, 3, 4, ...) ; the results are used for the calculation of the energy values of the alkali atoms. Section VII.3 gives a brief description of the solution of the Schr?dinger equation for the hydrogen atom, which is used for an alternative computation of the matr
57#
發(fā)表于 2025-3-31 12:57:42 | 只看該作者
Perturbation Theory, end of Section VIII.1 the Wigner-Brillouin and the Rayleigh-Schr?dinger perturbation expansions are obtained as special cases. Section VIII.2 applies this general procedure to the continuous spectrum and results in the Lippmann-Schwinger equation.
58#
發(fā)表于 2025-3-31 14:23:55 | 只看該作者
Electron Spin,on Hamiltonian for the spin interaction is determined in Section IX.3. In Section IX.3a the magnetic moment of the electron is determined by classical arguments; in Section IX.3b the magnetic field, which acts on the electron magnetic moment in an atom, is presented. In Section IX.4 these results ar
59#
發(fā)表于 2025-3-31 21:20:52 | 只看該作者
60#
發(fā)表于 2025-3-31 23:33:44 | 只看該作者
Some Fundamental Properties of Quantum Mechanics,experiment with the Stern-Gerlach apparatus it is shown that a polarized beam (a pure state) cannot be split by the magnetic field, and that the splitting of such a beam is a consequence of the measurement. In Section XIII.2 we derive the predictions of quantum mechanics for spin correlation measure
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