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Titlebook: Gauge Theory of Weak Interactions; Walter Greiner,Berndt Müller Textbook 20003rd edition Springer-Verlag Berlin Heidelberg 2000 Beta decay

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書目名稱Gauge Theory of Weak Interactions
編輯Walter Greiner,Berndt Müller
視頻videohttp://file.papertrans.cn/381/380943/380943.mp4
概述Carefully developed and well introduced text.Part of the Greiner lectures and its educational standards.Accessible introduction to the field.Now available as a newly revised edition.Includes supplemen
圖書封面Titlebook: Gauge Theory of Weak Interactions;  Walter Greiner,Berndt Müller Textbook 20003rd edition Springer-Verlag Berlin Heidelberg 2000 Beta decay
描述.Gauge Theory of Weak Interactions. treats the unification of electromagnetic and weak interactions and considers related phenomena. First, the Fermi theory of beta decay is presented, followed by a discussion of parity violation, clarifying the importance of symmetries. Then the concept of a spontaneously broken gauge theory is introduced, and all necessary mathematical tools are carefully developed. The "standard model" of unified electroweak interactions is thoroughly discussed including current developments. The final chapter contains an introduction to unified theories of strong and electroweak interactions. Numerous solved examples and problems make this volume uniquely suited as a text for an advanced course. This third edition has been carefully revised.
出版日期Textbook 20003rd edition
關(guān)鍵詞Beta decay; Elementary Particle Physics; Gauge Theory; Kaon; Lepton; Nuclear Physics; Weak Interactions; ha
版次3
doihttps://doi.org/10.1007/978-3-662-04211-3
isbn_ebook978-3-662-04211-3
copyrightSpringer-Verlag Berlin Heidelberg 2000
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The Neutral Kaon System,There are four strange pseudoscalar mesons K.,K.,K. and ., which are all eigenstates of the Hamiltonian of the strong interaction.
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https://doi.org/10.1007/978-3-658-11394-0, these are: the strong (nuclear) interaction, electromagnetism, the weak (nuclear) interaction, and gravity (see Table 1.1). The interaction strength varies with distance between the force centers. This is illustrated in the figure accompanying Table 1.1.
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https://doi.org/10.1007/978-3-322-88451-0ractions, and incorporating charged and neutral currents in a unified way. First we have to learn how to convert a theory involving massless vector bosons into a theory of massive particles, without disturbing the favourable high-energy behaviour of a massless propagator. We shall proceed by discuss
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https://doi.org/10.1007/978-3-658-27933-2aryon number . = 0), which always have integer spin. The lightest hadrons, with equal spin (and equal parity), can be arranged in simple multiplets, where two further quantum numbers serve as order criteria: the .,and its third component .., and the .,or alternatively the so-called strong . = . + ..
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