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11#
發(fā)表于 2025-3-23 09:42:47 | 只看該作者
12#
發(fā)表于 2025-3-23 17:54:49 | 只看該作者
13#
發(fā)表于 2025-3-23 18:26:33 | 只看該作者
14#
發(fā)表于 2025-3-23 23:59:44 | 只看該作者
15#
發(fā)表于 2025-3-24 02:56:52 | 只看該作者
Group Theory and Quantum Mechanics978-3-642-65860-0Series ISSN 0072-7830 Series E-ISSN 2196-9701
16#
發(fā)表于 2025-3-24 10:34:48 | 只看該作者
17#
發(fā)表于 2025-3-24 14:15:39 | 只看該作者
https://doi.org/10.1007/978-1-4612-2000-8A stationary state of a pair of electrons, without spin and without interaction, is determined by an eigenfunction of the form. in which .. and .. are the normed eigenfunctions of the single electrons. If .. and .. are their energy values, the energy of the whole system is ..
18#
發(fā)表于 2025-3-24 15:08:52 | 只看該作者
Groups and Their Representations,Any set of objects (called vectors) .,... that can be added and multiplied by real or complex numbers .,... will be called a . or ., provided the usual rules of addition and multiplication are satisfied:
19#
發(fā)表于 2025-3-24 19:54:07 | 只看該作者
20#
發(fā)表于 2025-3-24 23:25:36 | 只看該作者
The Spinning Electron,ng, it thus appears indispensible to assume, in addition to the magnetic moment of the orbital motion, another magnetic moment not depending on the orbital motion. According to the hypothesis of Uhlenbeck and Goudsmit, this moment arises from the so-called ., i.e. from the angular momentum of the “spinning” electron ..
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