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Titlebook: Quantum Physics; Florian Scheck Textbook 20071st edition Springer-Verlag Berlin Heidelberg 2007 Dirac equation.Heisenberg.Hilbert space.Pe

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發(fā)表于 2025-3-21 19:03:13 | 只看該作者 |倒序瀏覽 |閱讀模式
書目名稱Quantum Physics
編輯Florian Scheck
視頻videohttp://file.papertrans.cn/782/781404/781404.mp4
概述Complete introduction to quantum physics.Includes all mathematical details.Includes supplementary material:
圖書封面Titlebook: Quantum Physics;  Florian Scheck Textbook 20071st edition Springer-Verlag Berlin Heidelberg 2007 Dirac equation.Heisenberg.Hilbert space.Pe
描述.Scheck’s .Quantum Physics. presents a comprehensive introductory treatment, ideally suited for a two-semester course. Part One covers the basic principles and prime applications of quantum mechanics, from the uncertainty relations to many-body systems. Part Two introduces to relativistic quantum field theory and ranges from symmetries in quantum physics to electroweak interactions. Numerous worked-out examples as well as exercises, with solutions or hints, enables the book’s use as an accompanying text for courses,?and also for independent study. For both parts, the necessary mathematical framework is treated in adequate form and detail. The book ends with appendices covering mathematical fundamentals and enrichment topics, plus selected biographical notes on pioneers of quantum mechanics and quantum field theory..
出版日期Textbook 20071st edition
關(guān)鍵詞Dirac equation; Heisenberg; Hilbert space; Perturbation; Quantization; Quantum electrodynamics; Quantum th
版次1
doihttps://doi.org/10.1007/978-3-540-49972-5
isbn_ebook978-3-540-49972-5
copyrightSpringer-Verlag Berlin Heidelberg 2007
The information of publication is updating

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發(fā)表于 2025-3-21 22:33:55 | 只看該作者
Textbook 20071st editioniples and prime applications of quantum mechanics, from the uncertainty relations to many-body systems. Part Two introduces to relativistic quantum field theory and ranges from symmetries in quantum physics to electroweak interactions. Numerous worked-out examples as well as exercises, with solution
板凳
發(fā)表于 2025-3-22 01:44:46 | 只看該作者
Quantum Mechanics of Point Particlesh takes proper account of Planck’s quantum of action . and which encompasses classical mechanics, in the limit . → 0, but for which initially one has no more than the formal framework of canonical mechanics. This is to say, slightly exaggerating, that one tries to guess a theory for the hydrogen ato
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發(fā)表于 2025-3-22 06:27:46 | 只看該作者
Scattering of Particles by Potentialstions, contain important information about the physical systems that they describe. Yet, from a physicist’s point of view, the results obtained until now remain somewhat academic as long as we do not know how to render the information they contain visible by means of concrete experiments. For exampl
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Applications of Quantum Mechanicstopical problems. These methods which may be perturbative or nonperturbative, often are specific to the various disciplines, and it would go far beyond the scope of a textbook to discuss them extensively and in due detail. For instance, atomic and molecular physics make extensive use of . and of . t
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Quantized Fields and their Interpretation as the real scalar field, a Maxwell field, or some continuous mechanical system, when subject to the rules of quantum theory, turns into a field operator which can create or annihilate quanta of this field and which describes the kinematics and the spin properties of these quanta. This step allows
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Scattering Matrix and Observables in Scattering and Decaysquantum field theories that will be needed for the calculation of observables such as scattering cross sections and decay probabilities. The framework thus provided which rests on general, physically plausible assumptions, though fairly general is somewhat abstract. This is the reason why, in a firs
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Particles with Spin 1/2 and the Dirac Equationrmation behaviour of one-particle states. This prescription was one of the essential results of Chap. 6. Furthermore, the spin 1/2 (electrons, protons, other fermions) is decribed by the fundamental representation of the group .(2). The eigenstates of the observables . . and . . transform by the .-m
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