By Bugra Borasoy (auth.), Takhmasib Aliev, Namik Kemal Pak, Meltem Serin (eds.)
This quantity collects the edited educational lectures given on the moment foreign summer time tuition in excessive power Physics in Mgla, Turkey, in September 2006 - an annual occasion with foreign participation and a distinct specialise in paintings performed within the areas of valuable Asia.
With emphasis at the common version and past, lectures have been dedicated to offering an advent and replace to the various correct subject matters, akin to chiral perturbation idea, the Higgs mechanism, heavy flavour and b physics, CP violation, the AdS/CFT correspondence, principles on grand unification and neutrino physics and astrophysics
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Extra info for The Standard Model and Beyond: Proceedings of the 2nd International Summer School in High Energy Physics, Muğla, 25–30 September 2006
Rev. 183, 1245 (1969) S. Weinberg: Trans. NY Acad. Sci. 38, 185 (1977) J. Bijnens, G. Colangelo and G. Ecker: JHEP 9902, 020 (1999) I. Gerstein, R. Jackiw, B. W. Lee and S. Weinberg: Phys. Rev. D 3, 2486 (1971) J. Bijnens, G. Colangelo and G. Ecker: Annals Phys. , C. Aubin et al. [MILC Collaboration]: Phys. Rev. D 70, 114501 (2004) J. Bijnens, G. Ecker and J. Gasser: [arXiv:hep-ph/9411232] G. Ecker, J. Gasser, A. Pich and E. de Rafael: Nucl. Phys. B 321, 311 (1989); J. F. Donoghue, C. Ramirez and G.
L. Kane and S. Dawson, The Higgs Hunter’s Guide, Westview Press; New Ed. 2001. 7. The LEP Collaborations and LEP Higgs Working Group, ALEPH-2000-074 CONF 200-051. 8. M. Dittmar and S. pdf). 9. P. Nilles, Phys. Rept. 110, 1 (1984); M. E. Peskin, Supersymmetry: Theory, World Scientiﬁc, 1996; S. P. Martin, arXiv:hep-ph/9709356. 10. N. html); C. Csaki, J. Hubisz and P. Meade, arXiv:hep-ph/0510275. S. C. tw This note is based on several lectures on B physics, given to unspecialized students in particle physics.
The LEC L5 governs SU(3) breaking in the GB decay constants fK 4Lr = 1 + 25 (m2K − m2π ) + chiral logs . fπ f (100) Comparison with the experimental value  fK fπ ﬁxes Lr5 . 22 (101) exp Table 1. Phenomenological values and sources for the renormalized coupling constants Lri (µ = Mρ ) . 7 source fK /fπ m2K 0 − m2K + r2 π V π → eνγ Introduction to Chiral Perturbation Theory 23 The values of the Li can be understood in terms of meson resonance exchange . For resonance masses considerably larger than the involved p2 , the resonance propagators shrink to a single point and momenta, MR2 produce contact interactions of the chiral Lagrangian 1 1 → − 2 + O(p2 ) .
The Standard Model and Beyond: Proceedings of the 2nd International Summer School in High Energy Physics, Muğla, 25–30 September 2006 by Bugra Borasoy (auth.), Takhmasib Aliev, Namik Kemal Pak, Meltem Serin (eds.)