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Titlebook: Elements of Classical and Quantum Physics; Michele Cini Textbook 20181st edition Springer International Publishing AG, part of Springer Na

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發(fā)表于 2025-3-28 15:43:39 | 只看該作者
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發(fā)表于 2025-3-28 21:48:21 | 只看該作者
https://doi.org/10.1007/978-1-4842-6507-9isconceptions, when the common wisdom was that there is an absolute rest system and a force is needed to keep objects moving (However, the times were ripe and some of the works by Giordano Bruno (1548–1600) imply correct ideas about the relativity of motion). The worst difficulty was that the 2000-y
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發(fā)表于 2025-3-29 01:24:00 | 只看該作者
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發(fā)表于 2025-3-29 13:26:56 | 只看該作者
Make an E-commerce Site in a Weekendow, can be changed by canonical transformation, this statement implies that in Quantum Mechanics, we must enjoy the same freedom. We shall see later how this arises) Sometimes, there are complications due to the fact that some operators fail to commute; such cases will be noted below. Therefore, for
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發(fā)表于 2025-3-29 17:47:44 | 只看該作者
The Genesis and Development of MaT Projects,nally exposed to them. Some interesting one-particle problems in higher dimensions can be solved by separation of variables, thereby reducing them to 1d subproblems, and we shall encounter several examples in other chapters. However, in recent times there have been important technological developmen
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發(fā)表于 2025-3-29 20:35:43 | 只看該作者
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發(fā)表于 2025-3-30 02:51:30 | 只看該作者
https://doi.org/10.1007/978-3-8349-9479-0ntum operators, and we shall meet more. The scalar product of . with ., which is . may be regarded as the element . of some matrix . with . and . replaced by the indices . and . which are functions .; it is called a matrix element of .; the only real difference with a conventional matrix . is that t
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發(fā)表于 2025-3-30 08:04:34 | 只看該作者
Make-or-Buy bei Anwendungssystemenlar momentum, which has an eigenvalue equation depending on a single angle .. If . is an eigenstate belonging to a discrete eigenvalue ., .; in such cases, Quantum Mechanics gives certainties. Otherwise, after the measurement . . in an eigenstate of the operator, and if the measurement is repeated i
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