Download Strong Coupling Gauge Theories in LHC Era: Workshop in Honor by H Fukaya, M Harada, M Tanabashi, K Yamawaki PDF

By H Fukaya, M Harada, M Tanabashi, K Yamawaki

The aim of the Workshop is to have in depth discussions on either theoretical and phenomenological elements of sturdy coupling gauge theories (SCGTs), with specific emphasis at the version structures to be demonstrated within the LHC experiments. Dynamical concerns are mentioned in lattice simulations and numerous analytical tools. This court cases quantity is a suite of the displays made on the Workshop by way of many prime scientists within the box.

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Read or Download Strong Coupling Gauge Theories in LHC Era: Workshop in Honor of Toshihide Maskawa's 70th Birthday and 35th Anniversary of Dynamical Symmetry Breaking in SCGT PDF

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Non-Abelian vortices with general gauge groups One of the new results by us17 is the construction of non-Abelian vortex solutions based on a general gauge group G × U (1), where G = SU (N ), SO(N ), U Sp(2N ), etc. As in models based on SU (N ) gauge groups studied extensively in the last few years, we work with simple models which have the structure of the bosonic sector of N = 2 supersymmetric models. The model contains a FI (Fayet-Iliopoulos)-like term in the U (1) sector, allowing the system to develop stable vortices.

B 428, 105 (1998) [arXiv:hep-th/9802109]; E. Witten, Adv. Theor. Math. Phys. 2, 253 (1998) [arXiv:hepth/9802150]. 3. S. J. Brodsky, G. F. 3948 [hep-ph]. 4. A. Deur, V. Burkert, J. P. Chen and W. Korsch, Phys. Lett. 4119 [hep-ph]]. 5in 01-Brodsky 15 5. S. J. Brodsky and R. Shrock, Phys. Lett. 1535 [hep-th]]. 6. J. Polchinski and M. J. Strassler, Phys. Rev. Lett. 88, 031601 (2002) [arXiv:hepth/0109174]. 7. A. Karch, E. Katz, D. T. Son and M. A. Stephanov, Phys. Rev. D 74, 015005 (2006) [arXiv:hep-ph/0602229].

Even if the base point p is a perfectly generic, regular point of M, not close to any singularity, the field configurations in the transverse plane (S 2 ) trace the whole vacuum moduli space M. The energy distribution reflects the nontrivial structure of M as the volume of the target space is mapped into the transverse plane, C E=2 C ∂2K ¯ †J¯ = 2 ∂φI ∂φ ∂φI ∂φ†J¯ C ¯ ∂∂K . The field configuration may hit for instance one of the singularities (conic or not), or simply the regions of large scalar curvature.

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