By Elliot Leader, Enrico Predazzi
Chief and Predazzi have written an exsellent textual content for graduate scholars. They hide the big variety of subject matters in nice readability. specifically within the bankruptcy approximately renormalization they reach offering the center intimately with out technical obfuscation.
Read or Download An Introduction to Gauge Theories and Modern Particle Physics 2 Volume Hardback Set (Cambridge Monographs on Particle Physics, Nuclear Physics and Cosmology) (Vol.1) PDF
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Additional info for An Introduction to Gauge Theories and Modern Particle Physics 2 Volume Hardback Set (Cambridge Monographs on Particle Physics, Nuclear Physics and Cosmology) (Vol.1)
23), and of the leptons. Later, when we come to discuss intermediate vector mesons or gauge bosons which mediate the weak interactions, the picture will be altered to that in Fig. 6. 2 Pre-gauge theory of weak interactions 13 U U n=d d=p d u e Ve Fig. 4. Quark picture of neutron ,Q-decay. d u e Fig. 5. Quark level interaction responsible for 0-decay in Cabibbo theory. processes involving hadrons in these quark pictures, but it is best to think of them for the moment as a mnemonic for keeping track of quantum numbers and of the relative strengths of various reactions.
4. Diagram (b) requires the existence of a neutral vector boson in addition to the charged ones W±. , Ve W+ Ve and/or and/or L- (d) Fig. 4. Diagrams to cancel the bad behaviour of the graph in Fig. 3. existence of new leptons which would need to be heavy to explain their non-discovery. Note that L* cannot be a muon since we believe that lepton number is conserved. 8 GeV/c2 (see Chapter 14) which could only communicate with its own neutrino v,-. However, heavy leptons can also occur quite naturally in a gauge theory.
Formally one states that (e-, ve) have electron number +1, (e+, ve) have -1 and all other particles zero. Analogously (p-, vN,) have muon number +1, (p+, iN,) have -1 and all other particles zero. The validity of this structure is borne out by the absence of many reactions which would have been expected to be seen. Some examples are: 1. Absence of neutrinoless double /3-decay (Z, A) 74 (Z+2, A) + e- + ewhich would be kinematically favoured compared with the observed reaction (Z, A) -* (Z+2, A)+e-+e-+ve+1/e if it were possible to have the sequence, inside the nucleus n-* p+e- +ve ve+n +e- Typical half-lives for 2 neutrino double 0-decay are 1018-1020 years.
An Introduction to Gauge Theories and Modern Particle Physics 2 Volume Hardback Set (Cambridge Monographs on Particle Physics, Nuclear Physics and Cosmology) (Vol.1) by Elliot Leader, Enrico Predazzi