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Titlebook: Quantum Theory for Mathematicians; Brian C. Hall Textbook 2013 Springer Science+Business Media, LLC, part of Springer Nature 2013 Hilbert

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發(fā)表于 2025-3-21 19:43:42 | 只看該作者 |倒序?yàn)g覽 |閱讀模式
書目名稱Quantum Theory for Mathematicians
編輯Brian C. Hall
視頻videohttp://file.papertrans.cn/782/781501/781501.mp4
概述Explains physical ideas in the language of mathematics.Provides a self-contained treatment of the necessary mathematics, including spectral theory and Lie theory.Contains many exercises that will appe
叢書名稱Graduate Texts in Mathematics
圖書封面Titlebook: Quantum Theory for Mathematicians;  Brian C. Hall Textbook 2013 Springer Science+Business Media, LLC, part of Springer Nature 2013 Hilbert
描述.Although ideas from quantum physics play an important role in many parts of modern mathematics, there are few books about quantum mechanics aimed at mathematicians. This book introduces the main ideas of quantum mechanics in language familiar to mathematicians. Readers with little prior exposure to physics will enjoy the book‘s conversational tone as they delve into such topics as the Hilbert space approach to quantum theory; the Schr?dinger equation in one space dimension; the Spectral Theorem for bounded and unbounded self-adjoint operators; the Stone–von Neumann Theorem; the Wentzel–Kramers–Brillouin approximation; the role of Lie groups and Lie algebras in quantum mechanics; and the path-integral approach to quantum mechanics..The numerous exercises at the end of each chapter make the book suitable for both graduate courses and independent study. Most of the text is accessible to graduate students in mathematics who have had a first course in real analysis, covering the basics of L2 spaces and Hilbert spaces.? The final chapters introduce readers who are familiar with the theory of manifolds to more advanced topics, including geometric quantization..
出版日期Textbook 2013
關(guān)鍵詞Hilbert space; Lie groups; Stone-von Neumann theorem; WKB approximation; geometric quantization; quantum
版次1
doihttps://doi.org/10.1007/978-1-4614-7116-5
isbn_softcover978-1-4899-9362-5
isbn_ebook978-1-4614-7116-5Series ISSN 0072-5285 Series E-ISSN 2197-5612
issn_series 0072-5285
copyrightSpringer Science+Business Media, LLC, part of Springer Nature 2013
The information of publication is updating

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發(fā)表于 2025-3-21 21:39:23 | 只看該作者
A First Approach to Classical Mechanics,t just happens to lie in a line. We let .(.) denote the particle’s position as a function of time. The particle’s velocity is then . where we use a dot over a symbol to denote the derivative of that quantity with respect to the time ..
板凳
發(fā)表于 2025-3-22 02:24:35 | 只看該作者
A Particle in a Square Well, we made do in Chap.4 with solutions that are either approximate or that involve an integral that is not explicitly evaluated.) Usually, then, one analyzes the time-independent Schr?dinger equation (the eigenvector equation for .) and then attempts to infer something about the time-dependent problem
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Quantization Schemes for Euclidean Space,r . on the quantum Hilbert space.” The attentive reader will note that we have not, up to this point, given a general procedure for constructing . from ..If we call . the . of .,then we have only discussed the quantizations of a few very special classical observables, such as position, momentum, and
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發(fā)表于 2025-3-22 14:12:19 | 只看該作者
,The Stone–von Neumann Theorem,nt operators on . satisfying . Suppose also that . and . act irreducibly on .,meaning that the only closed subspaces of . invariant under . and . are {0} and ..Then provided that certain technical assumptions hold (the exponentiated commutation relations)
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發(fā)表于 2025-3-22 20:31:22 | 只看該作者
Lie Groups, Lie Algebras, and Representations, In many cases, the group of symmetries of a system is a ., that is, a group that is parameterized by one or more real parameters. More precisely, the symmetry group is often a ., that is, a smooth manifold endowed with a group structure in such a way that operations of inversion and group multiplic
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發(fā)表于 2025-3-23 00:28:28 | 只看該作者
Angular Momentum and Spin,l concept when a system has rotational symmetry, since in that case the angular momentum is a conserved quantity (Proposition 2.18). Quantum mechanically, angular momentum is still the “generator”of rotations, meaning that it is the infinitesimal generator of a one-parameter group of unitary rotatio
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