'Wilson loop' diaporamas de présentation

Holographic stringy hadrons

O. Aharony, O. Bergman, V. Kaplunovsky , S. Yankielowicz, B. Burrington, A. Dymarsky,G. Harpaz, N. Katz, U. Kol, Y. Kinar, S. Kuperstein, M. Kruczenski, D. Melnikov, O. Mintakevich, L. Pando-Zayas, K. Petters,U. Schreiber, S. Seki, D. Vaman, M. Zamaklar

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Entanglement Entropy in Holographic Superconductor Phase Transitions

Entanglement Entropy in Holographic Superconductor Phase Transitions . Rong -Gen Cai Institute of Theoretical Physics Chinese Academy of Sciences ( April 17 , 201 3 ). JHEP 1207 (2012) 088 ; JHEP 1207 (2012) 027 JHEP 1210 (2012) 107 ; arXiv: 1303.4828. Contents:.

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Recent developments in Monte Carlo studies of superstring theory

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Numerical tests of the gauge-gravity duality and beyond

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Simulating Superstrings inside a Black Hole

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Alexander Rothkopf Albert Einstein Center for Fundamental Physics

Heavy Quarkonia in the QGP from effective field theories and potentials. Alexander Rothkopf Albert Einstein Center for Fundamental Physics Institute for Theoretical Physics University of Bern. Hard Probes 2012, Cagliari, Italy May 30th 2012, 11:30 a.m.

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Non-relativistic string and D-branes on AdS 5 x S 5 from semiclassical approximation

?????????????? --- ??????????. 2007 ? 8 ? 9 ???????. Non-relativistic string and D-branes on AdS 5 x S 5 from semiclassical approximation. ?????? (KITP,UCSB). ??????? ( ?????? ) ???????. JHEP 0705 (2007) 051, hep-th/0703061 JHEP 0610 (2006) 078, hep-th/0605124. 1. ?????????.

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Proper Heavy Quark Potential from the Thermal Wilson Loop

Proper Heavy Quark Potential from the Thermal Wilson Loop. Alexander Rothkopf. In collaboration with T. Hatsuda and S. Sasaki see also arXiv:0910.2321. ???????????????????????????? ???????????????????????. Motivation. T ? 2 T C pQGP. T=2T C. or. T ? T C sQGP. T=T C.

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