Perturbative tests for a large-N reduced model of \( \mathcal{N} = {4} \) super Yang-Mills theory
- 34 Downloads
- 8 Citations
Abstract
We study a non-perturbative formulation of \( \mathcal{N} = {4} \) super Yang-Mills theory (SYM) on R × S 3 in the planar limit proposed in arXiv:0807.2352. This formulation is based on the large-N reduction, and the theory can be described as a particular large-N limit of the plane wave matrix model (PWMM), which is obtained by dimensionally reducing the original theory over S 3. In this paper, we perform some tests for this proposal. We construct an operator in the PWMM that corresponds to the Wilson loop in SYM in the continuum limit and calculate the vacuum expectation value of the operator for the case of the circular contour. We find that our result indeed agrees with the well-known result first obtained by Erickson, Semenoff and Zarembo. We also compute the beta function at the 1-loop level based on this formulation and see that it is indeed vanishing.
Keywords
Supersymmetric gauge theory AdS-CFT Correspondence Non-Commutative Geometry M(atrix) TheoriesReferences
- [1]J.M. Maldacena, The Large-N limit of superconformal field theories and supergravity, Adv. Theor. Math. Phys. 2 (1998) 231 [Int. J. Theor. Phys. 38 (1999) 1133] [hep-th/9711200] [INSPIRE].
- [2]S. Gubser, I.R. Klebanov and A.M. Polyakov, Gauge theory correlators from noncritical string theory, Phys. Lett. B 428 (1998) 105 [hep-th/9802109] [INSPIRE].MathSciNetADSGoogle Scholar
- [3]E. Witten, Anti-de Sitter space and holography, Adv. Theor. Math. Phys. 2 (1998) 253 [hep-th/9802150] [INSPIRE].MathSciNetzbMATHGoogle Scholar
- [4]N. Beisert et al., Review of AdS/CFT Integrability: An Overview, arXiv:1012.3982 [INSPIRE].
- [5]D.B. Kaplan and M. Ünsal, A Euclidean lattice construction of supersymmetric Yang-Mills theories with sixteen supercharges, JHEP 09 (2005) 042 [hep-lat/0503039] [INSPIRE].ADSCrossRefGoogle Scholar
- [6]M. Ünsal, Supersymmetric deformations of type IIB matrix model as matrix regularization of N =4 SYM, JHEP 04 (2006) 002 [hep-th/0510004] [INSPIRE].ADSCrossRefGoogle Scholar
- [7]J.W. Elliott, J. Giedt and G.D. Moore, Lattice four-dimensional N = 4 SYM is practical, Phys. Rev. D 78 (2008) 081701 [arXiv:0806.0013] [INSPIRE].MathSciNetADSGoogle Scholar
- [8]S. Catterall, First results from simulations of supersymmetric lattices, JHEP 01 (2009) 040 [arXiv:0811.1203] [INSPIRE].ADSCrossRefGoogle Scholar
- [9]J. Giedt, Progress in four-dimensional lattice supersymmetry, Int. J. Mod. Phys. A 24 (2009) 4045 [arXiv:0903.2443] [INSPIRE].MathSciNetADSGoogle Scholar
- [10]M. Hanada, S. Matsuura and F. Sugino, Two-dimensional lattice for four-dimensional N = 4 supersymmetric Yang-Mills, Prog. Theor. Phys. 126 (2011), 597–611 [arXiv:1004.5513] [INSPIRE].ADSCrossRefGoogle Scholar
- [11]M. Hanada, A proposal of a fine tuning free formulation of 4d N = 4 super Yang-Mills, JHEP 11 (2010) 112 [arXiv:1009.0901] [INSPIRE].ADSCrossRefGoogle Scholar
- [12]S. Catterall, E. Dzienkowski, J. Giedt, A. Joseph and R. Wells, Perturbative renormalization of lattice N = 4 super Yang-Mills theory, JHEP 04 (2011) 074 [arXiv:1102.1725] [INSPIRE].MathSciNetADSCrossRefGoogle Scholar
- [13]T. Ishii, G. Ishiki, S. Shimasaki and A. Tsuchiya, N = 4 Super Yang-Mills from the Plane Wave Matrix Model, Phys. Rev. D 78 (2008) 106001 [arXiv:0807.2352] [INSPIRE].MathSciNetADSGoogle Scholar
- [14]D.E. Berenstein, J.M. Maldacena and H.S. Nastase, Strings in flat space and pp waves from N =4 super Yang-Mills, JHEP 04 (2002)013 [hep-th/0202021] [INSPIRE].MathSciNetADSCrossRefGoogle Scholar
- [15]G. Ishiki, S. Shimasaki, Y. Takayama and A. Tsuchiya, Embedding of theories with SU(2–4) symmetry into the plane wave matrix model, JHEP 11 (2006) 089 [hep-th/0610038] [INSPIRE].MathSciNetADSCrossRefGoogle Scholar
- [16]T. Ishii, G. Ishiki, S. Shimasaki and A. Tsuchiya, Fiber Bundles and Matrix Models, Phys. Rev. D 77 (2008) 126015 [arXiv:0802.2782] [INSPIRE].MathSciNetADSGoogle Scholar
- [17]N. Kim, T. Klose and J. Plefka, Plane wave matrix theory from N = 4 super Yang-Mills on R × S 3, Nucl. Phys. B 671 (2003) 359 [hep-th/0306054] [INSPIRE].MathSciNetADSCrossRefGoogle Scholar
- [18]H. Lin, unpublished.Google Scholar
- [19]H. Lin and J.M. Maldacena, Fivebranes from gauge theory, Phys. Rev. D 74 (2006) 084014 [hep-th/0509235] [INSPIRE].MathSciNetADSGoogle Scholar
- [20]T. Eguchi and H. Kawai, Reduction of Dynamical Degrees of Freedom in the Large-N Gauge Theory, Phys. Rev. Lett. 48 (1982) 1063 [INSPIRE].ADSCrossRefGoogle Scholar
- [21]K.N. Anagnostopoulos, M. Hanada, J. Nishimura and S. Takeuchi, Monte Carlo studies of supersymmetric matrix quantum mechanics with sixteen supercharges at finite temperature, Phys. Rev. Lett. 100 (2008) 021601 [arXiv:0707.4454] [INSPIRE].ADSCrossRefGoogle Scholar
- [22]S. Catterall and T. Wiseman, Black hole thermodynamics from simulations of lattice Yang-Mills theory, Phys. Rev. D 78 (2008) 041502 [arXiv:0803.4273] [INSPIRE].MathSciNetADSGoogle Scholar
- [23]M. Honda, G. Ishiki, S.-W. Kim, J. Nishimura and A. Tsuchiya, in preparation.Google Scholar
- [24]J. Nishimura, Non-lattice simulation of supersymmetric gauge theories as a probe to quantum black holes and strings, PoS (LAT2009)016 [arXiv:0912.0327] [INSPIRE].
- [25]M. Honda, G. Ishiki, S.-W. Kim, J. Nishimura and A. Tsuchiya, Supersymmetry non-renormalization theorem from a computer and the AdS/CFT correspondence, PoS (Lattice 2010)253 [arXiv:1011.3904] [INSPIRE].
- [26]D. Berenstein and R. Cotta, A Monte-Carlo study of the AdS/CFT correspondence: An Exploration of quantum gravity effects, JHEP 04 (2007) 071 [hep-th/0702090] [INSPIRE].ADSCrossRefGoogle Scholar
- [27]D. Berenstein, R. Cotta and R. Leonardi, Numerical tests of AdS/CFT at strong coupling, Phys. Rev. D 78 (2008) 025008 [arXiv:0801.2739] [INSPIRE].MathSciNetADSGoogle Scholar
- [28]S. Catterall and G. van Anders, First Results from Lattice Simulation of the PWMM, JHEP 09 (2010) 088 [arXiv:1003.4952] [INSPIRE].ADSCrossRefGoogle Scholar
- [29]G. Ishiki, S.-W. Kim, J. Nishimura and A. Tsuchiya, Deconfinement phase transition in N =4 super Yang-Mills theory on R × S 3 from supersymmetric matrix quantum mechanics, Phys. Rev. Lett. 102 (2009) 111601 [arXiv:0810.2884] [INSPIRE].ADSCrossRefGoogle Scholar
- [30]G. Ishiki, S.-W. Kim, J. Nishimura and A. Tsuchiya, Testing a novel large-N reduction for N =4 super Yang-Mills theory on R × S 3, JHEP 09 (2009)029 [arXiv:0907.1488] [INSPIRE].MathSciNetADSCrossRefGoogle Scholar
- [31]Y. Kitazawa and K. Matsumoto, N = 4 Supersymmetric Yang-Mills on S 3 in Plane Wave Matrix Model at Finite Temperature, Phys. Rev. D 79 (2009) 065003 [arXiv:0811.0529] [INSPIRE].MathSciNetADSGoogle Scholar
- [32]G. Ishiki, S. Shimasaki and A. Tsuchiya, Large-N reduction for Chern-Simons theory on S 3, Phys. Rev. D 80 (2009) 086004 [arXiv:0908.1711] [INSPIRE].MathSciNetADSGoogle Scholar
- [33]G. Ishiki, S. Shimasaki and A. Tsuchiya, A Novel Large-N Reduction on S 3 : Demonstration in Chern-Simons Theory, Nucl. Phys. B 834 (2010) 423 [arXiv:1001.4917] [INSPIRE].MathSciNetADSGoogle Scholar
- [34]T. Ishii, G. Ishiki, K. Ohta, S. Shimasaki and A. Tsuchiya, On relationships among Chern-Simons theory, BF theory and matrix model, Prog. Theor. Phys. 119 (2008) 863 [arXiv:0711.4235] [INSPIRE].ADSzbMATHCrossRefGoogle Scholar
- [35]G. Ishiki, K. Ohta, S. Shimasaki and A. Tsuchiya, Two-Dimensional Gauge Theory and Matrix Model, Phys. Lett. B 672 (2009) 289 [arXiv:0811.3569] [INSPIRE].MathSciNetADSGoogle Scholar
- [36]M. Hanada, L. Mannelli and Y. Matsuo, Four-dimensional N = 1 super Yang-Mills from matrix model, Phys. Rev. D 80 (2009) 125001 [arXiv:0905.2995] [INSPIRE].MathSciNetADSGoogle Scholar
- [37]M. Hanada, L. Mannelli and Y. Matsuo, Large-N reduced models of supersymmetric quiver, Chern-Simons gauge theories and ABJM, JHEP 11 (2009) 087 [arXiv:0907.4937] [INSPIRE].MathSciNetADSCrossRefGoogle Scholar
- [38]H. Kawai, S. Shimasaki and A. Tsuchiya, Large-N reduction on group manifolds, Int. J. Mod. Phys. A 25 (2010) 3389 [arXiv:0912.1456] [INSPIRE].MathSciNetADSGoogle Scholar
- [39]H. Kawai, S. Shimasaki and A. Tsuchiya, Large-N reduction on coset spaces, Phys. Rev. D 81 (2010) 085019 [arXiv:1002.2308] [INSPIRE].MathSciNetADSGoogle Scholar
- [40]J.J. Heckman and H. Verlinde, Super Yang-Mills Theory as a Twistor Matrix Model, arXiv:1104.2605 [INSPIRE].
- [41]J. Erickson, G. Semenoff and K. Zarembo, Wilson loops in N = 4 supersymmetric Yang-Mills theory, Nucl. Phys. B 582 (2000) 155 [hep-th/0003055] [INSPIRE].MathSciNetADSCrossRefGoogle Scholar
- [42]N. Drukker and D.J. Gross, An Exact prediction of N = 4 SUSYM theory for string theory, J. Math. Phys. 42 (2001) 2896 [hep-th/0010274] [INSPIRE].MathSciNetADSzbMATHCrossRefGoogle Scholar
- [43]S.-J. Rey and J.-T. Yee, Macroscopic strings as heavy quarks in large-N gauge theory and anti-de Sitter supergravity, Eur. Phys. J. C 22 (2001) 379 [hep-th/9803001] [INSPIRE].MathSciNetADSCrossRefGoogle Scholar
- [44]J.M. Maldacena, Wilson loops in large-N field theories, Phys. Rev. Lett. 80 (1998) 4859 [hep-th/9803002] [INSPIRE].MathSciNetADSzbMATHCrossRefGoogle Scholar
- [45]D.E. Berenstein, R. Corrado, W. Fischler and J.M. Maldacena, The Operator product expansion for Wilson loops and surfaces in the large-N limit, Phys. Rev. D 59 (1999) 105023 [hep-th/9809188] [INSPIRE].MathSciNetADSGoogle Scholar
- [46]N. Drukker, D.J. Gross and H. Ooguri, Wilson loops and minimal surfaces, Phys. Rev. D 60 (1999) 125006 [hep-th/9904191] [INSPIRE].MathSciNetADSGoogle Scholar
- [47]V. Pestun, Localization of gauge theory on a four-sphere and supersymmetric Wilson loops, arXiv:0712.2824 [INSPIRE].
- [48]K. Dasgupta, M.M. Sheikh-Jabbari and M. Van Raamsdonk, Matrix perturbation theory for M-theory on a PP wave, JHEP 05 (2002) 056 [hep-th/0205185] [INSPIRE].ADSCrossRefGoogle Scholar
- [49]T. Banks, W. Fischler, S. Shenker and L. Susskind, M theory as a matrix model: A Conjecture, Phys. Rev. D 55 (1997) 5112 [hep-th/9610043] [INSPIRE].MathSciNetADSGoogle Scholar
- [50]N. Ishibashi, S. Iso, H. Kawai and Y. Kitazawa, Wilson loops in noncommutative Yang-Mills, Nucl. Phys. B 573 (2000) 573 [hep-th/9910004] [INSPIRE].MathSciNetADSzbMATHCrossRefGoogle Scholar
- [51]K. Okuyama, N = 4 SYM on R × S 3 and PP wave, JHEP 11 (2002) 043 [hep-th/0207067] [INSPIRE].ADSGoogle Scholar
- [52]G. Ishiki, Y. Takayama and A. Tsuchiya, N = 4 SYM on R × S 3 and theories with 16 supercharges, JHEP 10 (2006) 007 [hep-th/0605163] [INSPIRE].MathSciNetADSCrossRefGoogle Scholar
- [53]H. Grosse, C. Klimč´ık and P. Prešnajder, Topologically nontrivial field configurations in noncommutative geometry, Commun. Math. Phys. 178 (1996) 507 [hep-th/9510083] [INSPIRE].ADSzbMATHCrossRefGoogle Scholar
- [54]S. Baez, A. Balachandran, B. Ydri and S. Vaidya, Monopoles and solitons in fuzzy physics, Commun. Math. Phys. 208 (2000) 787 [hep-th/9811169] [INSPIRE].MathSciNetADSzbMATHCrossRefGoogle Scholar
- [55]J. Hoppe, Quantum Theory of a Massless Relativistic Surface and a Two-Dimensional Bound State Problem, Ph.D. Thesis, Massachusetts Institute of Technology, Camebridge U.K. (1988).Google Scholar
- [56]B. de Wit, J. Hoppe and H. Nicolai, On the Quantum Mechanics of Supermembranes, Nucl. Phys. B 305 (1988) 545 [INSPIRE].ADSCrossRefGoogle Scholar
- [57]J. Hoppe, Diffeomorphism groups, quantization and SU(∞), Int. J. Mod. Phys. A 4 (1989) 5235 [INSPIRE].MathSciNetADSGoogle Scholar
- [58]D. Varshalovich, A. Moskalev and V. Khersonskii, Quantum Theory of Angular Momentum, World Scientific, Singapore (1988).Google Scholar
- [59]G. Ishiki, Matrix regularization of N = 4 SYM on R × S 3, Int. J. Mod. Phys. A 23 (2008) 2199 [INSPIRE].MathSciNetADSGoogle Scholar
- [60]A. Tsuchiya, Fiber bundle and matrix models, Int. J. Mod. Phys. A 23 (2008) 2165 [INSPIRE].MathSciNetADSGoogle Scholar