2007
DOI: 10.1088/1126-6708/2007/11/085
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Holographic phase transitions at finite chemical potential

Abstract: Recently holographic techniques have been used to study the thermal properties of N = 2 super-Yang-Mills theory, with gauge group SU (N c ) and coupled to N f ≪ N c flavours of fundamental matter, at large N c and large 't Hooft coupling. Here we consider the phase diagram as a function of temperature and baryon chemical potential µ b . For fixed µ b < N c M q there is a line of first order thermal phase transitions separating a region with vanishing baryon density and one with nonzero density. For fixed µ b >… Show more

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Cited by 113 publications
(150 citation statements)
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“…In particular, there are unstable regions in the phase diagrams. Studies of finite chemical potential and finite density effects for D7 brane probes in the AdS-Schwarzschild background may be found in [101,[202][203][204][205][206][207][208][209][210].…”
Section: More Thermodynamicsmentioning
confidence: 99%
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“…In particular, there are unstable regions in the phase diagrams. Studies of finite chemical potential and finite density effects for D7 brane probes in the AdS-Schwarzschild background may be found in [101,[202][203][204][205][206][207][208][209][210].…”
Section: More Thermodynamicsmentioning
confidence: 99%
“…As an example we consider here spectral functions at finite temperature and the quark chemical potential as discussed in [209]. The phase diagram was found in [202,205] and is displayed in fig. 29.…”
Section: More Thermodynamicsmentioning
confidence: 99%
“…together with the constitutive equation for the energy-momentum tensor 52) with the (internal) energy density ǫ, the pressure P The constitutive equation (3.52) is obtained by writing down all possible terms in an expansion in powers of spatial derivatives of hydrodynamic variables to leading order. We can also include the next to leading order yielding…”
Section: Relativistic Hydrodynamicsmentioning
confidence: 99%
“…In this context we will review the thermodynamics at finite U(1) baryon density [42] or finite baryon chemical potential [52] in section 4.3. Investigating the effects of isospin and the non-Abelian part of the flavor group we will develop the thermodynamics for the non-Abelian part SU(N f ) of the full flavor gauge symmetry U(N f ).…”
Section: Holographic Thermo-and Hydrodynamicsmentioning
confidence: 99%
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