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Anti-de Sitter space, thermal phase transition, and confinement in gauge theories (1998)

by E Witten
Venue:Adv. Theor. Math. Phys
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Large N field theories, string theory and gravity

by Ofer Aharony, Steven S. Gubser, Juan Maldacena, Hirosi Ooguri, Yaron Oz , 2001
"... We review the holographic correspondence between field theories and string/M theory, focusing on the relation between compactifications of string/M theory on Anti-de Sitter spaces and conformal field theories. We review the background for this correspondence and discuss its motivations and the evide ..."
Abstract - Cited by 1443 (45 self) - Add to MetaCart
We review the holographic correspondence between field theories and string/M theory, focusing on the relation between compactifications of string/M theory on Anti-de Sitter spaces and conformal field theories. We review the background for this correspondence and discuss its motivations and the evidence for its correctness. We describe the main results that have been derived from the correspondence in the regime that the field theory is approximated by classical or semiclassical gravity. We focus on the case of the N = 4 supersymmetric gauge theory in four dimensions, but we discuss also field theories in other dimensions, conformal and non-conformal, with or without supersymmetry, and in particular the relation to QCD. We also discuss some implications for black hole physics.
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...sence of phase transitions). This will be discussed in section 4.3. There are many more qualitative tests of the correspondence, such as the existence of confinement for the finite temperature theory =-=[185]-=-, which we will not discuss in this section. We will also not discuss here tests involving the behavior of the theory on its moduli space [169, 186, 170]. 2 Unlike most of the other tests described he...

Mirror Manifolds and Topological Field Theory

by Edward Witten - in Essays on Mirror Manifolds (ed. S.T. Yau), International Press, Hong Kong , 1992
"... In N = 4 super Yang-Mills theory on a four-manifold M, one can specify a discrete magnetic flux valued in H2 (M,ZN). This flux is encoded in the AdS/CFT correspondence in terms of a five-dimensional topological field theory with Chern-Simons action. A similar topological field theory in seven dimens ..."
Abstract - Cited by 380 (12 self) - Add to MetaCart
In N = 4 super Yang-Mills theory on a four-manifold M, one can specify a discrete magnetic flux valued in H2 (M,ZN). This flux is encoded in the AdS/CFT correspondence in terms of a five-dimensional topological field theory with Chern-Simons action. A similar topological field theory in seven dimensions governs the space of “conformal blocks ” of the six-dimensional (0, 2) conformal field theory. December
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... of X, namely X1 = S1 × B4 and X2 = B2 ×S3 (here Bn denotes an ndimensional ball); many important properties of Yang-Mills theory at nonzero temperature are reflected in the behavior of these two X’s =-=[12]-=-. This example has H2 (M,ZN) = 0 and so does not serve as a good illustration of the issues explored in the present paper. But one can readily modify it to give an example with nontrivial discrete mag...

Renormalization group flows from holography -- Supersymmetry and a c-theorem

by D. Z. Freedman, S. S. Gubser, K. Pilch, N. P. Warner - ADV THEOR. MATH. PHYS , 1999
"... We obtain first order equations that determine a supersymmetric kink solution in fivedimensional N = 8 gauged supergravity. The kink interpolates between an exterior anti-de Sitter region with maximal supersymmetry and an interior anti-de Sitter region with one quarter of the maximal supersymmetry. ..."
Abstract - Cited by 294 (25 self) - Add to MetaCart
We obtain first order equations that determine a supersymmetric kink solution in fivedimensional N = 8 gauged supergravity. The kink interpolates between an exterior anti-de Sitter region with maximal supersymmetry and an interior anti-de Sitter region with one quarter of the maximal supersymmetry. One eighth of supersymmetry is preserved by the kink as a whole. We interpret it as describing the renormalization group flow in N = 4 super-Yang-Mills theory broken to an N = 1 theory by the addition of a mass term for one of the three adjoint chiral superfields. A detailed correspondence is obtained between fields of bulk supergravity in the interior anti-de Sitter region and composite operators of the infrared field theory. We also point out that the truncation used to find the reduced symmetry critical point can be extended to obtain a new N = 4 gauged supergravity theory holographically dual to a sector of N = 2 gauge theories based on quiver diagrams. We consider more general kink geometries and construct a c-function that is positive and monotonic if a weak energy condition holds in the bulk gravity theory. For even-dimensional boundaries, the c-function coincides with the trace anomaly coefficients of the holographically related field theory in limits where conformal invariance is recovered.

Energy loss of a heavy quark moving through N = 4 supersymmetric Yang-Mills plasma

by C. P. Herzog, A. Karch, P. Kovtun, C. Kozcaz, L. G. Yaffe , 2006
"... ..."
Abstract - Cited by 231 (10 self) - Add to MetaCart
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Holographic duality with a view toward many-body physics

by John McGreevy , 2009
"... These are notes based on a series of lectures given at the KITP workshop Quantum Criticality and the AdS/CFT Correspondence in July, 2009. The goal of the lectures was to introduce condensed matter physicists to the AdS/CFT correspondence. Discussion of string theory and of supersymmetry is avoided ..."
Abstract - Cited by 150 (2 self) - Add to MetaCart
These are notes based on a series of lectures given at the KITP workshop Quantum Criticality and the AdS/CFT Correspondence in July, 2009. The goal of the lectures was to introduce condensed matter physicists to the AdS/CFT correspondence. Discussion of string theory and of supersymmetry is avoided to the extent possible.
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...dition on the bulk wave equation at the IR end of the geometry. The problem becomes like QM of a 1d particle trapped at both ends, and therefore has a discrete spectrum. There exist gravity solutions =-=[53, 19, 54]-=- which are dual to field theories with logarithmically running couplings which become strong in the IR, leading to a gap to almost all excitations (except some order N0 number of Goldstone bosons), as...

Holographic phase transitions at finite baryon density

by Shinpei Kobayashi, David Mateos, Shunji Matsuura, Robert C. Myers, Rowan M. Thomson , 2007
"... ..."
Abstract - Cited by 139 (13 self) - Add to MetaCart
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Aspects of Holographic Entanglement Entropy

by Shinsei Ryu, Tadashi Takayanagi
"... This is an extended version of our short report hep-th/0603001, where a holographic interpretation of entanglement entropy in conformal field theories is proposed from AdS/CFT correspondence. In addition to a concise review of relevant recent progresses of entanglement entropy and details omitted in ..."
Abstract - Cited by 126 (4 self) - Add to MetaCart
This is an extended version of our short report hep-th/0603001, where a holographic interpretation of entanglement entropy in conformal field theories is proposed from AdS/CFT correspondence. In addition to a concise review of relevant recent progresses of entanglement entropy and details omitted in the earlier letter, this paper includes the following several new results: We give a more direct derivation of our claim which relates the entanglement entropy with the minimal area surfaces in the AdS3/CFT2 case as well as some further discussions on higher dimensional cases. Also the relation between the entanglement entropy and central charges in 4D conformal field theories is examined. We check that the logarithmic part of the 4D entanglement entropy computed in the CFT side agrees with the AdS5 result at least under a specific condition. Finally we estimate the entanglement entropy of massive theories in generic dimensions by making use of our proposal.
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...vention is such that S11Dsugra = 1 2κ 2 11 407.5 Finite Temperature Case Consider the N = 4 super Yang-Mills theory on R 4 at finite temperature T. This system is dual to the AdS black hole geometry =-=[25, 69]-=- ds 2 = R 2 [ 2 du hu2 + u2 ( −hdt 2 + dx 2 1 + dx22 + dx2 ] ) 2 3 + dΩ5 , (7.33) where h = 1 − u4 0 u 4, u0 = πT. (7.34) Various analyzes show that this theory has properties of a confining gauge the...

Holographic Entanglement Entropy: An Overview

by Tatsuma Nishioka , Shinsei Ryu , Tadashi Takayanagi , 2009
"... In this article, we review recent progresses on the holographic understandings of the entanglement entropy in the AdS/CFT correspondence. After reviewing the general idea of holographic entanglement entropy, we will explain its applications to confinement/deconfinement phase transitions, black hole ..."
Abstract - Cited by 120 (12 self) - Add to MetaCart
In this article, we review recent progresses on the holographic understandings of the entanglement entropy in the AdS/CFT correspondence. After reviewing the general idea of holographic entanglement entropy, we will explain its applications to confinement/deconfinement phase transitions, black hole entropy and covariant formulation of holography.

The AdS/CFT Correspondence and a New Positive Energy Conjecture for General Relativity

by Gary T. Horowitz, Robert C. Myers , 1998
"... We examine the AdS/CFT correspondence when the gauge theory is considered on a compactified space with supersymmetry breaking boundary conditions. We find that the corresponding supergravity solution has a negative energy, in agreement with the expected negative Casimir energy in the field theory. S ..."
Abstract - Cited by 115 (12 self) - Add to MetaCart
We examine the AdS/CFT correspondence when the gauge theory is considered on a compactified space with supersymmetry breaking boundary conditions. We find that the corresponding supergravity solution has a negative energy, in agreement with the expected negative Casimir energy in the field theory. Stability of the gauge theory would imply that this supergravity solution has minimum energy among all solutions with the same boundary conditions. Hence we are lead to conjecture a new positive energy theorem for asymptotically locally Anti-de Sitter spacetimes. We show that the candidate minimum energy solution is stable against all quadratic fluctuations of the metric.
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... For solutions which approach AdS globally, there are positive energy theorems which ensure that this energy cannot be negative [5], in agreement with the stability of the gauge theory vacuum. Witten =-=[6]-=- has suggested that one can describe ordinary (i.e., nonsupersymmetric) Yang-Mills gauge theory by compactifying one direction on a circle and requiring antiperiodic boundary conditions for the fermio...

Exploring improved holographic theories for QCD

by U. Gürsoy, E. Kiritsis, F. Nitti - Part I”, [ArXiv:0707.1324
"... Abstract: This paper is a continuation of ArXiv:0707.1324 where improved holographic theories for QCD were set up and explored. Here, the IR confining geometries are classified and analyzed. They all end in a “good ” (repulsive) singularity in the IR. The glueball spectra are gaped and discrete, and ..."
Abstract - Cited by 115 (15 self) - Add to MetaCart
Abstract: This paper is a continuation of ArXiv:0707.1324 where improved holographic theories for QCD were set up and explored. Here, the IR confining geometries are classified and analyzed. They all end in a “good ” (repulsive) singularity in the IR. The glueball spectra are gaped and discrete, and they favorably compare to the lattice data. Quite generally, confinement and discrete spectra imply each other. Asymptotically linear glueball masses can also be achieved. Asymptotic mass ratios of various glueballs with different spin also turn out to be universal. Mesons dynamics is implemented via space filling D4 − ¯ D4 brane pairs. The associated tachyon dynamics is analyzed and chiral symmetry breaking is shown. The dynamics of the RR axion is analyzed, and the non-perturbative running of the QCD θ-angle is obtained. It is shown to always vanish in the IR.
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...ptures the leading behavior of the quark-antiquark potential. In QCD the first subleading correction is the Lüscher term, ∼ 1/L. As shown in [14], this term arises in some confining backgrounds (e.g. =-=[13]-=-) from the first quantum corrections to the classical Wilson loop in [12]. It would be interesting to see if this is also the case in the models we are considering.– 13 – 3.2 Confining IR asymptotics...

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