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Journal articles on the topic 'Dualité AdS/CFT'

Author: Grafiati

Published: 4 June 2021

Last updated: 19 February 2022

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1

SCHWARZ, JOHN H. "RECENT PROGRESS IN AdS/CFT." International Journal of Modern Physics A 25, no. 02n03 (January 30, 2010): 310–18. http://dx.doi.org/10.1142/s0217751x10048639.

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The study of AdS/CFT (or gauge/gravity) duality has been one of the most active and illuminating areas of research in string theory over the past decade. The scope of its relevance and the insights it is providing seem to be ever expanding. In this talk I briefly describe some of the attempts to explore how the duality works for maximally supersymmetric systems.

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2

Peschanski, R. "Regge amplitudes from AdS/CFT duality." Nuclear Physics B - Proceedings Supplements 117 (April 2003): 849–54. http://dx.doi.org/10.1016/s0920-5632(03)90690-6.

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3

Hansen, James, and Per Kraus. "S-duality in AdS/CFT magnetohydrodynamics." Journal of High Energy Physics 2009, no. 10 (October 19, 2009): 047. http://dx.doi.org/10.1088/1126-6708/2009/10/047.

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4

Berenstein, David, and Robert G. Leigh. "Discrete torsion, AdS/CFT and duality." Journal of High Energy Physics 2000, no. 01 (January 26, 2000): 038. http://dx.doi.org/10.1088/1126-6708/2000/01/038.

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5

Beccaria, M., and C. Ortix. "AdS/CFT duality at strong coupling." Theoretical and Mathematical Physics 152, no. 2 (August 2007): 1060–68. http://dx.doi.org/10.1007/s11232-007-0090-4.

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6

Natsuume, Makoto. "Critical Phenomena in the AdS/CFT Duality." Progress of Theoretical Physics Supplement 186 (October 1, 2010): 491–97. http://dx.doi.org/10.1143/ptps.186.491.

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7

Karanikas, A. I., and C. N. Ktorides. "Zig zag symmetry in AdS/CFT duality." European Physical Journal C 54, no. 1 (January 11, 2008): 159–68. http://dx.doi.org/10.1140/epjc/s10052-007-0504-3.

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8

BROWER, RICHARD C. "AdS/CFT DUALITY AND THE GLUEBALL SPECTRUM." International Journal of Modern Physics A 16, supp01c (September 2001): 1005–7. http://dx.doi.org/10.1142/s0217751x01008722.

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The complete glueball spectrum for the AdS7 black hole supergravity dual of QCD is shown to bare a striking resemblance to the known lattice results despite the limitations of the strong coupling approximation. Further extensions of duality to couple hadronic matter to gravity in the Randall-Sundram brane world scenario are suggested.

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9

Brodsky, Stanley J., and Guy F. de Téramond. "Applications of AdS/CFT Duality to QCD." International Journal of Modern Physics A 21, no. 04 (February 10, 2006): 762–68. http://dx.doi.org/10.1142/s0217751x06032009.

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Even though quantum chromodynamics is a broken conformal theory, the AdS/CFT correspondence has led to important insights into the properties of QCD. For example, as shown by Polchinski and Strassler, dimensional counting rules for the power-law falloff of hadron scattering amplitudes follow from dual holographic models with conformal behavior at short distances and confinement at large distances. We find that one also obtains a remarkable representation of the entire light-quark meson and baryon spectrum, including all orbital excitations, based on only one mass parameter. We also show how hadron light-front wavefunctions and hadron form factors in both the space-like and time-like regions can be predicted.

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10

Pahlavani, M. R., and R. Morad. "Application of AdS/CFT in Nuclear Physics." Advances in High Energy Physics 2014 (2014): 1–19. http://dx.doi.org/10.1155/2014/863268.

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We review some recent progress in studying the nuclear physics especially nucleon-nucleon (NN) force within the gauge-gravity duality, in context of noncritical string theory. Our main focus is on the holographic QCD model based on the AdS6background. We explain the noncritical holography model and obtain the vector-meson spectrum and pion decay constant. Also, we study the NN interaction in this frame and calculate the nucleonmeson coupling constants. A further topic covered is a toy model for calculating the light nuclei potential. In particular, we calculate the light nuclei binding energies and also excited energies of some available excited states. We compare our results with the results of other nuclear models and also with the experimental data. Moreover, we describe some other issues which are studied using the gauge-gravity duality.

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11

HUSAIN, VIQAR. "NAKED SINGULARITIES AND THE WILSON LOOP." Modern Physics Letters A 17, no. 15n17 (June 7, 2002): 955–65. http://dx.doi.org/10.1142/s021773230200693x.

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We give observations about dualities where one of the dual theories is geometric. These are illustrated with a duality between the simple harmonic oscillator and a topological field theory. We then discuss the Wilson loop in the context of the AdS/CFT duality. We show that the Wilson loop calculation for certain asymptotically AdS scalar field space–times with naked singularities gives results qualitatively similar to that for the AdS black hole. In particular, it is apparent that (dimensional) metric parameters in the singular space–times permit a "thermal screening" interpretation for the uark potential in the boundary theory, just like black hole mass. This suggests that the Wilson loop calculation merely captures metric parameter information rather than true horizon information.

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12

Puletti, Valentina Giangreco Marotta. "On String Integrability: A Journey through the Two-Dimensional Hidden Symmetries in the AdS/CFT Dualities." Advances in High Energy Physics 2010 (2010): 1–133. http://dx.doi.org/10.1155/2010/471238.

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One of the main topics in the modern String Theory are the AdS/CFT dualities. Proving such conjectures is extremely difficult since the gauge and string theory perturbative regimes do not overlap. In this perspective, the discovery of infinitely many conserved charges, that is, the integrability, in the planar AdS/CFT has allowed us to reach immense progresses in understanding and confirming the duality. We review the fundamental concepts and properties of integrability in two-dimensionalσ-models and in the AdS/CFT context. The first part is focused on theAdS5/CFT4duality, especially the classical and quantum integrability of the type IIB superstring onAdS5×S5which is discussed in both pure spinor and Green-Schwarz formulations. The second part is dedicated to theAdS4/CFT3duality with particular attention to the type IIA superstring onAdS4×ℂP3and its integrability. This review is based on the author's PhD thesis discussed at Uppsala University the 21st September 2009.

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13

Goldberger, Walter D. "AdS/CFT duality for non-relativistic field theory." Journal of High Energy Physics 2009, no. 03 (March 10, 2009): 069. http://dx.doi.org/10.1088/1126-6708/2009/03/069.

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14

Frampton, Paul H., and William F. Shively. "Conformal gauge theories from AdS/CFT superstring duality?" Physics Letters B 454, no. 1-2 (May 1999): 49–52. http://dx.doi.org/10.1016/s0370-2693(99)00359-7.

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15

Barbón, J. L. F., and A. Pasquinucci. "Aspects of instanton dynamics in AdS/CFT duality." Physics Letters B 458, no. 2-3 (July 1999): 288–96. http://dx.doi.org/10.1016/s0370-2693(99)00607-3.

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16

Minic, Djordje, and Michel Pleimling. "The Jarzynski identity and the AdS/CFT duality." Physics Letters B 700, no. 3-4 (June 2011): 277–81. http://dx.doi.org/10.1016/j.physletb.2011.05.021.

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17

Rickles, Dean. "AdS/CFT duality and the emergence of spacetime." Studies in History and Philosophy of Science Part B: Studies in History and Philosophy of Modern Physics 44, no. 3 (August 2013): 312–20. http://dx.doi.org/10.1016/j.shpsb.2012.06.001.

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18

BOUHMADI, MARIAN, LUIS J. GARAY, and PEDRO F. GONZÁLEZ-DÍAZ. "CREATION OF OPEN UNIVERSES AND CFT/AdS DUALITY." Modern Physics Letters A 16, no. 07 (March 7, 2001): 403–9. http://dx.doi.org/10.1142/s021773230100367x.

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By replacing the singularity of the Hawking–Turok instanton for a regular asymptotically anti-de Sitter Euclidean wormhole, we conjecture that there may exist a holographic duality between CFT on the boundary of anti-de Sitter space and the Lorentzian isotropic open universes obtained by continuing the wormhole instanton according to the Hawking–Turok prescription.

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19

Dorn, H., and H. J. Otto. "OnQQ¯-potentials Derived via the AdS/CFT Duality." Fortschritte der Physik 48, no. 1-3 (January 2000): 93–98. http://dx.doi.org/10.1002/(sici)1521-3978(20001)48:1/3<93::aid-prop93>3.0.co;2-d.

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20

Chu, Chong-Sun, and Pei-Ming Ho. "Time-dependent AdS/CFT duality and null singularity." Journal of High Energy Physics 2006, no. 04 (April 6, 2006): 013. http://dx.doi.org/10.1088/1126-6708/2006/04/013.

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21

CADONI, M., and P. CARTA. "TACHYONS IN DE SITTER SPACE AND ANALYTICAL CONTINUATION FROM dS/CFT TO AdS/CFT." International Journal of Modern Physics A 19, no. 29 (November 20, 2004): 4985–5001. http://dx.doi.org/10.1142/s0217751x0401821x.

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We discuss analytic continuation from d-dimensional Lorentzian de Sitter ( dS d) to d-dimensional Lorentzian anti-de Sitter ( AdS d) space–time. We show that AdS d, with opposite signature of the metric, can be obtained as analytic continuation of a portion of dS d. This implies that the dynamics of (positive square-mass) scalar particles in AdS d can be obtained from the dynamics of tachyons in dS d. We discuss this correspondence both at the level of the solution of the field equations and of the Green functions. The AdS / CFT duality is obtained as analytic continuation of the dS / CFT duality.

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22

Chesler, Paul M., and Wilke van der Schee. "Early thermalization, hydrodynamics and energy loss in AdS/CFT." International Journal of Modern Physics E 24, no. 10 (October 2015): 1530011. http://dx.doi.org/10.1142/s0218301315300118.

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Gauge/gravity duality has provided unprecedented opportunities to study dynamics in certain strongly coupled gauge theories. This review aims to highlight several applications to heavy ion collisions including far-from-equilibrium dynamics, hydrodynamics and jet energy loss at strong coupling.

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23

Sin, Sang-Jin, and Ismail Zahed. "Ampere's law and energy loss in AdS/CFT duality." Physics Letters B 648, no. 4 (May 2007): 318–22. http://dx.doi.org/10.1016/j.physletb.2007.01.074.

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24

Hollowood, Timothy J., and Valentin V. Khoze. "ADHM and D-instantons in orbifold AdS/CFT duality." Nuclear Physics B 575, no. 1-2 (May 2000): 78–106. http://dx.doi.org/10.1016/s0550-3213(00)00086-9.

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25

Lunin, Oleg, and Samir D. Mathur. "AdS/CFT duality and the black hole information paradox." Nuclear Physics B 623, no. 1-2 (February 2002): 342–94. http://dx.doi.org/10.1016/s0550-3213(01)00620-4.

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26

Chu, Chong-Sun, Shou-Huang Dai, and Douglas J. Smith. "AdS/CFT duality for non-anticommutative supersymmetric gauge theory." Journal of High Energy Physics 2008, no. 05 (May 9, 2008): 029. http://dx.doi.org/10.1088/1126-6708/2008/05/029.

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27

Pu, Shi, and Qun wang. "Bjorken hydrodynamics with radial flow in AdS/CFT duality." Nuclear Physics A 834, no. 1-4 (March 2010): 269c—272c. http://dx.doi.org/10.1016/j.nuclphysa.2009.12.056.

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28

Gremm, Martin, and Anton Kapustin. "N = 1 theories, T-duality, and AdS/CFT correspondence." Journal of High Energy Physics 1999, no. 07 (July 2, 1999): 005. http://dx.doi.org/10.1088/1126-6708/1999/07/005.

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29

FRAMPTON, PAUL H. "AdS/CFT DUALITY AND CONFORMALITY FOR NON-ABELIAN ORBIFOLD." International Journal of Modern Physics A 16, supp01c (September 2001): 975–77. http://dx.doi.org/10.1142/s0217751x01008643.

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30

HOVDEBO, JORDAN L., MARTÍN KRUCZENSKI, DAVID MATEOS, ROBERT C. MYERS, and DAVID J. WINTERS. "HOLOGRAPHIC MESONS: ADDING FLAVOR TO THE ADS/CFT DUALITY." International Journal of Modern Physics A 20, no. 15 (June 20, 2005): 3428–33. http://dx.doi.org/10.1142/s0217751x05026728.

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We study mesons in an [Formula: see text] super Yang-Mills theory with fundamental matter from its dual string theory on AdS5 × S5 with a D7-brane probe. For quarks with a finite mass mq, the meson spectrum is discrete and exhibits a mass gap of order [Formula: see text]. The spectrum of mesons with large spin J is obtained from semiclassical rotating open strings attached to the D7-brane. It displays Regge behaviour for [Formula: see text] whereas for [Formula: see text] it corresponds to that of two non-relativistic quarks bound by a Coulomb potential. We calculate 〈 Tr F2〉 around an isolated quark, to gain insight into the Regge behaviour of the spinning mesons.

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31

Frolov, S., and A. A. Tseytlin. "Rotating string solutions: AdS/CFT duality in non-supersymmetric sectors." Physics Letters B 570, no. 1-2 (September 2003): 96–104. http://dx.doi.org/10.1016/j.physletb.2003.07.022.

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32

Frampton, Paul H., and Thomas W. Kephart. "Chiral fermions and AdS/CFT duality for a nonabelian orbifold." Physics Letters B 485, no. 4 (July 2000): 403–7. http://dx.doi.org/10.1016/s0370-2693(00)00700-0.

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33

Guralnik, Z., S. Kovacs, and B. Kulik. "AdS/CFT duality and the Higgs branch of  = 2 SYM." Fortschritte der Physik 53, no. 5-6 (May 13, 2005): 480–85. http://dx.doi.org/10.1002/prop.200510207.

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34

Erdmenger, Johanna, Johannes Große, and Zachary Guralnik. "Spectral flow on the Higgs branch and AdS/CFT duality." Journal of High Energy Physics 2005, no. 06 (June 20, 2005): 052. http://dx.doi.org/10.1088/1126-6708/2005/06/052.

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35

McGreevy, John. "Holographic Duality with a View Toward Many-Body Physics." Advances in High Energy Physics 2010 (2010): 1–54. http://dx.doi.org/10.1155/2010/723105.

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These are notes based on a series of lectures given at the KITP workshopQuantum Criticality and the AdS/CFT Correspondencein 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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36

MAMEDOV, SHAHIN, and SHAHROKH PARVIZI. "AdS/CFT CORRESPONDENCE VIA R-CURRENT CORRELATION FUNCTIONS REVISITED." International Journal of Modern Physics A 23, no. 22 (September 10, 2008): 3721–45. http://dx.doi.org/10.1142/s0217751x08039943.

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Motivated by realizing open/closed string duality in the work by Gopakumar [Phys. Rev. D70, 025009 (2004)], we study two- and three-point correlation functions of R-current vector fields in [Formula: see text] super-Yang–Mills theory. These correlation functions in free field limit can be derived from the worldline formalism and are written as heat kernel integrals in the position space. We show that reparametrizing these integrals converts them to the expected AdS supergravity results which are known in terms of bulk to boundary propagators. We expect that this reparametrization corresponds to transforming open string moduli parametrization to the closed string ones.

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37

Marolf, Donald, and Simo F. Ross. "Boundary conditions and dualities: vector fields in AdS/CFT." Journal of High Energy Physics 2006, no. 11 (November 29, 2006): 085. http://dx.doi.org/10.1088/1126-6708/2006/11/085.

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38

Berkooz, Micha. "A proposal on some microscopic aspects of the AdS/CFT duality." Nuclear Physics B 553, no. 1-2 (July 1999): 205–30. http://dx.doi.org/10.1016/s0550-3213(99)00220-5.

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39

Costa, Miguel S. "A test of the AdS/CFT duality on the Coulomb branch." Physics Letters B 482, no. 1-3 (June 2000): 287–92. http://dx.doi.org/10.1016/s0370-2693(00)00484-6.

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40

Guo, Er-Dong, Miao Li, and Jia-Rui Sun. "CFT dual of charged AdS black hole in the large dimension limit." International Journal of Modern Physics D 25, no. 07 (June 2016): 1650085. http://dx.doi.org/10.1142/s0218271816500851.

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We study the dual CFT description of the [Formula: see text]-dimensional Reissner–Nordström-Anti de Sitter (RN-AdS[Formula: see text]) black hole in the large dimension (large [Formula: see text]) limit, both for the extremal and nonextremal cases. The central charge of the dual CFT2 (or chiral CFT1) is calculated for the near-horizon near extremal geometry which possesses an AdS2 structure. Besides, the [Formula: see text]-picture hidden conformal symmetry in the nonextremal background can be naturally obtained by a probe charged scalar field in the large [Formula: see text] limit, without the need to input the usual limits to probe the hidden conformal symmetry. Furthermore, a new dual CFT description of the nonextremal RN-AdS[Formula: see text] black hole is found in the large [Formula: see text] limit and the duality is analyzed by comparing the entropies, the absorption cross-sections and the retarded Green’s functions obtained both from the gravity and the dual CFT sides.

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41

Chowdhury, Borun D. "Limitations of holography." International Journal of Modern Physics D 24, no. 01 (December 28, 2014): 1550008. http://dx.doi.org/10.1142/s021827181550008x.

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By studying global AdS using different foliations, global and Rindler-AdS, we show that there are two different asymptotic Fefferman–Graham expansions possible and thus two different definitions of "boundaries". We demonstrate that imposing boundary conditions on the two boundaries is not mutually compatible even when these boundaries are pushed to infinity. Thus, these two procedures define two genuinely distinct theories that we call global-CFT and Rindler-CFT. We show that the Rindler-CFT is not the same as the theory one gets by "Rindlerizing the global-CFT" described in hep-th/9804085. We conjecture that the Rindler theory is incapable of capturing the dynamics inside the horizon and discuss its implications for the BTZ-CFT duality proposed in hep-th/0106112.

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42

Bitaghsir Fadafan, K., and S. Mojarad Laman jouee. "Study of the Brownian motion of heavy particles using AdS/CFT duality." Iranian Journal of Physics Research 18, no. 2 (September 1, 2018): 190–94. http://dx.doi.org/10.29252/ijpr.18.2.190.

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43

CHANDRASEKHAR, B., and BINATA PANDA. "BRANE EMBEDDINGS IN ${\rm AdS}_4 \times {\mathcal{CP}}^3$." International Journal of Modern Physics A 26, no. 14 (June 10, 2011): 2377–404. http://dx.doi.org/10.1142/s0217751x1105347x.

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We construct D-brane embeddings in [Formula: see text] by studying the consistency conditions following from the pull back of target space equations of motion. We explicitly discuss the supersymmetry preserved by these embeddings by analyzing the compatibility of kappa symmetry projections with the target space Killing spinors in each case. The embeddings correspond to AdS/dCFT dualities involving ABJM theories with a defect. We also comment on the defect CFT.

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44

Nigam, Rahul. "A Review of Conformal Field Theory in 2D." JOURNAL OF ADVANCES IN PHYSICS 6, no. 2 (December 2, 2014): 1079–105. http://dx.doi.org/10.24297/jap.v6i2.1784.

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In this review we study the elementary structure of Conformal Field Theory in which is a recipe for further studies of critical behavior of various systems in statistical mechanics and quantum field theory. We briefly review CFT in dimensions which plays a prominent role for example in the well-known duality AdS/CFT in string theory where the CFT lives on the AdS boundary. We also describe the mapping of the theory from the cylinder to a complex plane which will help us gain an insight into the process of radial quantization and radial ordering. Finally we will develop the representation of the Virasoro algebra which is the well-known "Verma module".Â Â

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45

Itsios, Georgios, Carlos Núñez, Konstadinos Sfetsos, and Daniel C. Thompson. "Non-Abelian T-duality and the AdS/CFT correspondence: New N=1 backgrounds." Nuclear Physics B 873, no. 1 (August 2013): 1–64. http://dx.doi.org/10.1016/j.nuclphysb.2013.04.004.

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46

Costa, Miguel S. "Erratum to: “A test of the AdS/CFT duality on the Coulomb branch”." Physics Letters B 489, no. 3-4 (September 2000): 439. http://dx.doi.org/10.1016/s0370-2693(00)00939-4.

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47

Awad, Adel. "Five-Dimensional Kerr–AdS Black Holes, First Law and Counterterms." International Journal of Modern Physics A 22, no. 31 (December 20, 2007): 5700–5708. http://dx.doi.org/10.1142/s0217751x07038931.

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Using counterterm subtraction technique we calculate the action and other thermodynamical quantities for the general Kerr–AdS black hole in five dimensions. We show that the resulting thermodynamical quantities do satisfy the first law of thermodynamics upon choosing the non-rotating Einstein space as a boundary. Furthermore, the vacuum energies and conformal anomalies calculated from both sides of the AdS/CFT duality match exactly. Comparing this result to previous known results, one is lead to raise the question: why some choices of the boundary metric produce quantities that do not satisfy the first law? Answering such a question will help us understand the relevance of the AdS vacuum energy on the gravity side.

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48

de Boer, Jan, Andrea Pasquinucci, and Kostas Skenderis. "$\mathrm{AdS}$/$\mathrm{CFT}$ dualities involving large $2d N=4$ superconformal symmetry." Advances in Theoretical and Mathematical Physics 3, no. 3 (1999): 577–614. http://dx.doi.org/10.4310/atmp.1999.v3.n3.a5.

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49

Dorn, H., and V. D. Pershin. "Concavity of the potential in super Yang-Mills gauge theory and AdS/CFT duality." Physics Letters B 461, no. 4 (September 1999): 338–44. http://dx.doi.org/10.1016/s0370-2693(99)00821-7.

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50

Vecchia, Paolo Di, Jens Lyng Petersen, Michela Petrini, Rodolfo Russo, and Alessandro Tanzini. "The three-string vertex and the AdS/CFT duality in the PP-wave limit." Classical and Quantum Gravity 21, no. 9 (April 2, 2004): 2221–40. http://dx.doi.org/10.1088/0264-9381/21/9/001.

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