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000291907 1001_ $$0P:(DE-HGF)0$$aHanada, Masanori$$b0$$eCorresponding author
000291907 1112_ $$aPanic2014$$cHamburg$$d2014-08-25 - 2014-08-29$$gPanic2014$$wGermany
000291907 245__ $$aWhy does black hole describe the deconfinement phase?
000291907 260__ $$aHamburg$$bDeutsches Elektronen-Synchrotron, DESY$$c2014
000291907 300__ $$a637-640
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000291907 520__ $$aIn the gauge/gravity duality, the deconfinement transition in the gauge theory is identified with the formation of black hole in the dual gravity theory. By assuming this correspondence, many predictions on QGP have been made. In this talk, we justify this approach quantitatively, and also provide an intuitive understanding. Firstly we give quantitative evidence for this identification from the thermodynamic study of the supersymmetric theory. We show that string theory and gauge theory give the same answer, even at finite temperature, including the $1/N$ correction. Then we consider generic gauge theories and show that the deconfinement transition is the condensation of very long and self-intersecting QCD strings, which is analogous to the formation of a black hole in string theory.
000291907 536__ $$0G:(DE-HGF)POF3-611$$a611 - Fundamental Particles and Forces (POF3-611)$$cPOF3-611$$fPOF III$$x0
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000291907 650_7 $$2INSPIRE$$agravitation: duality
000291907 650_7 $$2INSPIRE$$ablack hole: formation
000291907 650_7 $$2INSPIRE$$aquantum chromodynamics: string
000291907 650_7 $$2INSPIRE$$agauge field theory
000291907 650_7 $$2INSPIRE$$adeconfinement
000291907 650_7 $$2INSPIRE$$afinite temperature
000291907 650_7 $$2INSPIRE$$athermodynamical
000291907 650_7 $$2INSPIRE$$asupersymmetry
000291907 650_7 $$2INSPIRE$$acondensation
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000291907 773__ $$a10.3204/DESY-PROC-2014-04/160
000291907 7870_ $$0PUBDB-2015-03603$$aSchmidt, Alexander et.al.$$dHamburg : Deutsches Elektronen-Synchrotron, DESY, Hamburg, 2014$$iIsPartOf$$rDESY-PROC-2014-04$$tProceedings, 20th International Conference on Particles and Nuclei (PANIC 14)
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