By P. Urban (auth.), Prof. Dr. Paul Urban (eds.)

Weak interactions and better symmetries are these days of specified value for simple debris concept. in recent years either theoretical and experimental physicists grew to become an increasing number of attracted to the topic. a result of advanced topic and the scarce on hand literature right introductions within the topic are tiresome. The mathematical again­ flooring reminiscent of greater Algebra and Grouptheory and so forth. can't be utilized instantly in all circumstances. The 3rd Schladming college classes at the above topic belong to this class. the current first complement quantity of "Acta Physica Austriaca" includes all lectures (with literature references) giving not just a overview of the basics but additionally discussing fresh examine paintings. I ,;incerely wish that the book will locate readers. within the final years it turned commonplace in physics and arithmetic to rearrange summer time faculties on topics which permit the skilled in addition to the younger scientiflt to get speedy conversant in exact glossy fields. Discussions and personal contacts make sure that individuals to the touch speedy the peripheries of the topic in query, and new examine paintings can be influenced which another way couldn't be anticipated. Graz, October, 1964.

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Additional resources for Weak Interactions and Higher Symmetries: Proceedings of the III. Internationale Hochschulwochen für Kernphysik 1964 der Karl-Franzens-Universität Graz, at Schladming (Steiermark, Austria) 24th February – 7th March 1964

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The electromagnetic currents may now written as and it = 13, (D3 + -i= Ds) 13 i; yfL Bj; + since the currents should depend linearly on Q, Q = 1+ Y /2 =F 3 1/V3Fs or D3 1/V3 Ds. The mass differences due to the electromagnetic interaction may now be computed. These mass differences will depend on the algebraic quantities: + + (F3+V'~ Fsr. (F3+~}Fs) (D3+jI~Ds), and M. E. 58 MAYER: since we are looking at the graph 888 Fig. 18 ++ + (F3 + V~Fsr. where there are 2 electronmagnetic couplings on this one line, we need jf1 j~L.

2. , Helvetia Physica Acta 30, 409 (1957). 3. , Proceedings of the 1962 International Conference on High-Energy Physics at CERN, CERN, Geneva p. 325. 4. , Annals of Physics 2, 407 (1957). 5. , Physical Review 106, 1296 (1957). 6. , and J. C. POLKINGHORNE, Nuovo cimento 2, 685 (1955). 7. SAKURAI, J. , Annals of Physics 11, 1 (1960). 8. YANG, C. , and R. L. :MILLS, Physical Review 96, 191 (1954). 9. :MAYER, :M. , Nuovo cimento 11, 760 (1959). 10. , Progress of Theoretical Physics 16, 686 (1956). 11.

For protons and neutrons, kaons, and pions there is no symmetry in the primitive sense that we could replace a proton by a neutron or a kaon by a pion (not only is the set I, I a, Y different from proton to neutron, kaon to pion, but also the mass). We consider super-multiplets of baryons and pseudoscalar mesons where the degenerate mass of all baryons is the same and of all pseudoscalar mesons the same. We then look for symmetry breaking interactions to account for the observed mass spectrum. 2.

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