Advertisement

Journal of High Energy Physics

, 2011:36 | Cite as

Perturbative tests for a large-N reduced model of \( \mathcal{N} = {4} \) super Yang-Mills theory

  • Goro Ishiki
  • Shinji ShimasakiEmail author
  • Asato Tsuchiya
Article

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) Theories 

References

  1. [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. [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. [3]
    E. Witten, Anti-de Sitter space and holography, Adv. Theor. Math. Phys. 2 (1998) 253 [hep-th/9802150] [INSPIRE].MathSciNetzbMATHGoogle Scholar
  4. [4]
    N. Beisert et al., Review of AdS/CFT Integrability: An Overview, arXiv:1012.3982 [INSPIRE].
  5. [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. [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. [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. [8]
    S. Catterall, First results from simulations of supersymmetric lattices, JHEP 01 (2009) 040 [arXiv:0811.1203] [INSPIRE].ADSCrossRefGoogle Scholar
  9. [9]
    J. Giedt, Progress in four-dimensional lattice supersymmetry, Int. J. Mod. Phys. A 24 (2009) 4045 [arXiv:0903.2443] [INSPIRE].MathSciNetADSGoogle Scholar
  10. [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. [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. [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. [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. [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. [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. [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. [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. [18]
    H. Lin, unpublished.Google Scholar
  19. [19]
    H. Lin and J.M. Maldacena, Fivebranes from gauge theory, Phys. Rev. D 74 (2006) 084014 [hep-th/0509235] [INSPIRE].MathSciNetADSGoogle Scholar
  20. [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. [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. [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. [23]
    M. Honda, G. Ishiki, S.-W. Kim, J. Nishimura and A. Tsuchiya, in preparation.Google Scholar
  24. [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. [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. [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. [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. [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. [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. [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. [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. [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. [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. [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. [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. [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. [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. [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. [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. [40]
    J.J. Heckman and H. Verlinde, Super Yang-Mills Theory as a Twistor Matrix Model, arXiv:1104.2605 [INSPIRE].
  41. [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. [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. [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. [44]
    J.M. Maldacena, Wilson loops in large-N field theories, Phys. Rev. Lett. 80 (1998) 4859 [hep-th/9803002] [INSPIRE].MathSciNetADSzbMATHCrossRefGoogle Scholar
  45. [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. [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. [47]
    V. Pestun, Localization of gauge theory on a four-sphere and supersymmetric Wilson loops, arXiv:0712.2824 [INSPIRE].
  48. [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. [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. [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. [51]
    K. Okuyama, N = 4 SYM on R × S 3 and PP wave, JHEP 11 (2002) 043 [hep-th/0207067] [INSPIRE].ADSGoogle Scholar
  52. [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. [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. [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. [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. [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. [57]
    J. Hoppe, Diffeomorphism groups, quantization and SU(∞), Int. J. Mod. Phys. A 4 (1989) 5235 [INSPIRE].MathSciNetADSGoogle Scholar
  58. [58]
    D. Varshalovich, A. Moskalev and V. Khersonskii, Quantum Theory of Angular Momentum, World Scientific, Singapore (1988).Google Scholar
  59. [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. [60]
    A. Tsuchiya, Fiber bundle and matrix models, Int. J. Mod. Phys. A 23 (2008) 2165 [INSPIRE].MathSciNetADSGoogle Scholar

Copyright information

© SISSA, Trieste, Italy 2011

Authors and Affiliations

  • Goro Ishiki
    • 1
    • 2
  • Shinji Shimasaki
    • 2
    • 3
    Email author
  • Asato Tsuchiya
    • 4
  1. 1.Center for Quantum Spacetime (CQUeST)Sogang UniversitySeoulRepublic of Korea
  2. 2.Department of PhysicsKyoto UniversityKyotoJapan
  3. 3.Harish-Chandra Research InstituteAllahabadIndia
  4. 4.Department of PhysicsShizuoka UniversityShizuokaJapan

Personalised recommendations