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Titlebook: Relativistic Particle Physics; Hartmut M. Pilkuhn Textbook 1979 Springer-Verlag Berlin Heidelberg 1979 Dirac equation.Elementarteilchen.Qu

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樓主: Encomium
11#
發(fā)表于 2025-3-23 10:10:33 | 只看該作者
https://doi.org/10.1007/978-3-642-88079-7Dirac equation; Elementarteilchen; Quantenelektrodynamik; Relativistische Quantenmechanik; mechanics; qua
12#
發(fā)表于 2025-3-23 15:03:15 | 只看該作者
978-3-642-88081-0Springer-Verlag Berlin Heidelberg 1979
13#
發(fā)表于 2025-3-23 19:24:21 | 只看該作者
Relativistic Particle Physics978-3-642-88079-7Series ISSN 1864-5879 Series E-ISSN 1864-5887
14#
發(fā)表于 2025-3-24 00:33:16 | 只看該作者
15#
發(fā)表于 2025-3-24 02:21:01 | 只看該作者
Particular Electromagnetic Processes in Collisions with Atoms and Nuclei,ectron emission). Typical energy losses in single collisions . (. characterizes the final state of the excited target) are much smaller than the kinetic energy of particle .. The particle then moves approximately on a straight line, with an energy loss per target density ..
16#
發(fā)表于 2025-3-24 09:56:49 | 只看該作者
17#
發(fā)表于 2025-3-24 13:24:50 | 只看該作者
Textbook 1979ms the basis of many other sciences, and relativistic particle physics forms the basis of physics. Starting from nonrelativistic point mechanics, there are three major steps: first to classical (unquantized) relativistic electrodynamics, then to non- relativistic quantum mechanics and finally to rel
18#
發(fā)表于 2025-3-24 17:21:05 | 只看該作者
Radiation and Quantum Electrodynamics,t only if .. is interpreted as an operator which can create and annihilate photons. As explained in section 2–8, gauge invariance permits us to impose the condition div . = 0 on this operator. Since we wish to keep classical electric and magnetic fields as well, we put ..
19#
發(fā)表于 2025-3-24 19:16:49 | 只看該作者
20#
發(fā)表于 2025-3-25 02:34:26 | 只看該作者
Radiation and Quantum Electrodynamics,ses in which photons are emitted or absorbed. For example, if an excited atom |..> has been formed by a rapid collision at a certain time, the probability amplitude of finding the atom in the state |..> decreases afterwards, and new states |..> |...> appear, in which the atom is in states of lower e
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