Titlebook: Gauge Theory of Weak Interactions; Walter Greiner,Berndt Müller Textbook 2009Latest edition Springer-Verlag Berlin Heidelberg 2009 Element

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https://doi.org/10.1007/978-3-662-29339-3ys 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 isospin ., and its third component .., and the strangeness ., or alternatively the so-called strong hypercharge .=.+..

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https://doi.org/10.1007/978-3-663-04720-9 In order to describe the weak interactions of the hadrons themselves we must in addition know how the hadrons are made up of quarks, that is, we must know the wave functions of the quarks within the hadrons. This problem has not yet been completely solved, but there are a number of models which ref

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https://doi.org/10.1007/978-3-662-35318-9ent shows that K. and K. form a conjugate particle–antiparticle pair, as does the pair K. and .. While both K. and . are neutral, they differ in the signs of isospin and strangeness. We know that isospin and strangeness conservation are violated by the weak interaction. Thus, despite the fact that K

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https://doi.org/10.1007/978-3-663-07096-2treats leptons and quarks on the same footing. However, the fact that leptons carry integer charge while the charge of quarks is 1/3 is needed as a basic input. On the other hand, there are indications that this fact is due to some superior principle, that is a larger symmetry. This leads to the hyp

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978-3-540-87842-1Springer-Verlag Berlin Heidelberg 2009

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Walter Greiner,Berndt MüllerCarefully 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

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