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Titlebook: Elementary Particle Physics; Concepts and Phenome Otto Nachtmann Textbook 1990 Springer-Verlag Berlin Heidelberg 1990 Particle Physics.elem

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发表于 2025-3-21 18:57:36 | 显示全部楼层 |阅读模式
书目名称Elementary Particle Physics
副标题Concepts and Phenome
编辑Otto Nachtmann
视频video
丛书名称Theoretical and Mathematical Physics
图书封面Titlebook: Elementary Particle Physics; Concepts and Phenome Otto Nachtmann Textbook 1990 Springer-Verlag Berlin Heidelberg 1990 Particle Physics.elem
描述This book grew-how could it be otherwise?-out of a series oflectures which the author held at the University of Heidelberg. The purpose ofthese lectures was to give an introduction to the phenomenology of elementary particles for students both of theoretical and experimental orientation. With the present book the author has set himself the same aim. The reader is assumed to be familiar with ordinary nonrelativistic quantum mechanics as presented, e.g., in the following books: Quantum Mechanics, by L.1. Schiff (McGraw-Hill, New York, 1955); Quantum Mechanics, Vol. I, by K. Gottfried (W.A. Benjamin, Reading, Ma., 1966). The setup of the present book is as follows. In the first part we present some basic general principles and concepts which are used in elementary particle physics. The reader is supposed to learn here the "language" of particle physics. An introductory chapter deals with special relativity, of such funda­ mental importance for particle physics, which most ofthe time is high energy, i.e., highly relativistic physics. Further chapters of this first part deal with the Dirac equation, with the theory of quantized fields, and with the general definitions of the scattering
出版日期Textbook 1990
关键词Particle Physics; elementary particle physics; mechanics; quantum mechanics; relativity; special relativi
版次1
doihttps://doi.org/10.1007/978-3-642-61281-7
isbn_softcover978-3-540-51647-7
isbn_ebook978-3-642-61281-7Series ISSN 1864-5879 Series E-ISSN 1864-5887
issn_series 1864-5879
copyrightSpringer-Verlag Berlin Heidelberg 1990
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The Theory of Special Relativity and Relativistic Kinematicsas it occurs when a beam of protons from an accelerator impinges on a target (Fig. 2.1.). If the energy of the incident protons is large enough, then as a result of Einstein’s equivalence relationship between mass and energy (Einstein 1905b), it is possible for the kinetic energy of the original pro
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Particles and Fieldse appropriate formalism for describing the quantum behavior of elementary particles is the . founded by Dirac, Jordan, Pauli, and Heisenberg (Dirac 1927; Jordan 1928; Heisenberg 1929,1930). An important feature of this theory is that it unites wave- and particle-like aspects. For example, quantum fi
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The Scattering Matrix and the Scattering Cross-Sectionprocesses or decay and production of particles. The central role here is played by the scattering matrix ., which was introduced by Wheeler and Heisenberg (Wheeler 1937; Heisenberg 1943, 1944). Before presenting a general formulation we will look at a simple example.
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Radiative Correctionsperiment. We know, however, that, in principle the theory includes higher order terms and that for a precise comparison with experiment, these too must be taken into account. After the development of QED at the end of the 1920s, it quickly became clear that in calculations of higher order terms, the
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Historical Overviewf quantum chromodynamics (QCD), which lays claim to being the fundamental theory in this area of physics. In this part of the book we will attempt to trace the historical path which led to QCD. Despite the existence of some impressive comparisons between experimental data and QCD, it should be stres
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Textbook 1990ecial relativity, of such funda­ mental importance for particle physics, which most ofthe time is high energy, i.e., highly relativistic physics. Further chapters of this first part deal with the Dirac equation, with the theory of quantized fields, and with the general definitions of the scattering
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Linking Methods in Critical Point Theoryse of light quanta, the situation was exactly the reverse. The wave nature of light was a dogma of the nineteenth century. It was only with the discovery of the photoelectric effect that physicists were forced to think again. The revolutionary idea of Einstein—the hypothesis of light quanta, in whic
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