Advertisement

Journal of High Energy Physics

, 2011:20 | Cite as

Direct test of the gauge-gravity correspondence for Matrix theory correlation functions

  • Masanori HanadaEmail author
  • Jun Nishimura
  • Yasuhiro Sekino
  • Tamiaki Yoneya
Article

Abstract

We study correlation functions in (0 + 1)-dimensional maximally supersym-metric U(N ) Yang-Mills theory, which was proposed by Banks et al. as a non-perturbative definition of 11-dimensional M-theory in the infinite-momentum frame. We perform first-principle calculations using Monte Carlo simulations, and compare the results against the predictions obtained previously based on the gauge-gravity correspondence from 10 dimensions. After providing a self-contained review on these predictions, we present clear evidence that the predictions in the large-N limit actually hold even at small N such as N =2 and 3. The predicted behavior seems to continue to the far infrared regime, which goes beyond the naive range of validity of the 10D supergravity analysis. This suggests that the correlation functions also contain important information on the M-theory limit.

Keywords

Gauge-gravity correspondence M(atrix) Theories Nonperturbative Effects 

References

  1. [1]
    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].ADSMathSciNetGoogle Scholar
  2. [2]
    W. Taylor, M(atrix) theory: matrix quantum mechanics as a fundamental theory, Rev. Mod. Phys. 73 (2001) 419 [hep-th/0101126] [INSPIRE].CrossRefzbMATHADSGoogle Scholar
  3. [3]
    E. Witten, String theory dynamics in various dimensions, Nucl. Phys. B 443 (1995) 85 [hep-th/9503124] [INSPIRE].CrossRefADSMathSciNetGoogle Scholar
  4. [4]
    C. Hull and P. Townsend, Unity of superstring dualities, Nucl. Phys. B 438 (1995) 109 [hep-th/9410167] [INSPIRE].CrossRefADSMathSciNetGoogle Scholar
  5. [5]
    E. Witten, Bound states of strings and p-branes, Nucl. Phys. B 460 (1996) 335 [hep-th/9510135] [INSPIRE].CrossRefADSMathSciNetGoogle Scholar
  6. [6]
    B. de Wit, J. Hoppe and H. Nicolai, On the quantum mechanics of supermembranes, Nucl. Phys. B 305 (1988) 545 [INSPIRE].CrossRefADSGoogle Scholar
  7. [7]
    Y. Okawa and T. Yoneya, Multi-body interactions of D-particles in supergravity and matrix theory, Nucl. Phys. B 538 (1999) 67 [hep-th/9806108] [INSPIRE].CrossRefADSMathSciNetGoogle Scholar
  8. [8]
    Y. Okawa and T. Yoneya, Equations of motion and Galilei invariance in D-particle dynamics, Nucl. Phys. B 541 (1999) 163 [hep-th/9808188] [INSPIRE].CrossRefADSMathSciNetGoogle Scholar
  9. [9]
    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].zbMATHADSMathSciNetGoogle Scholar
  10. [10]
    N. Itzhaki, J.M. Maldacena, J. Sonnenschein and S. Yankielowicz, Supergravity and the large-N limit of theories with sixteen supercharges, Phys. Rev. D 58 (1998) 046004 [hep-th/9802042] [INSPIRE].ADSMathSciNetGoogle Scholar
  11. [11]
    A. Jevicki and T. Yoneya, Space-time uncertainty principle and conformal symmetry in D-particle dynamics, Nucl. Phys. B 535 (1998) 335 [hep-th/9805069] [INSPIRE].CrossRefADSMathSciNetGoogle Scholar
  12. [12]
    A. Jevicki, Y. Kazama and T. Yoneya, Generalized conformal symmetry in D-brane matrix models, Phys. Rev. D 59 (1999) 066001 [hep-th/9810146] [INSPIRE].ADSMathSciNetGoogle Scholar
  13. [13]
    Y. Sekino and T. Yoneya, Generalized AdS/CFT correspondence for matrix theory in the large-N limit, Nucl. Phys. B 570 (2000) 174 [hep-th/9907029] [INSPIRE].CrossRefADSMathSciNetGoogle Scholar
  14. [14]
    Y. Sekino, Supercurrents in matrix theory and the generalized AdS/CFT correspondence, Nucl. Phys. B 602 (2001) 147 [hep-th/0011122] [INSPIRE].CrossRefADSMathSciNetGoogle Scholar
  15. [15]
    S. Gubser, I.R. Klebanov and A.M. Polyakov, Gauge theory correlators from non-critical string theory, Phys. Lett. B 428 (1998) 105 [hep-th/9802109] [INSPIRE].ADSMathSciNetGoogle Scholar
  16. [16]
    E. Witten, Anti-de Sitter space and holography, Adv. Theor. Math. Phys. 2 (1998) 253 [hep-th/9802150] [INSPIRE].zbMATHMathSciNetGoogle Scholar
  17. [17]
    D.N. Kabat and W. Taylor, Linearized supergravity from matrix theory, Phys. Lett. B 426 (1998) 297 [hep-th/9712185] [INSPIRE].ADSMathSciNetGoogle Scholar
  18. [18]
    W. Taylor and M. Van Raamsdonk, Supergravity currents and linearized interactions for matrix theory configurations with fermionic backgrounds, JHEP 04 (1999) 013 [hep-th/9812239] [INSPIRE].ADSGoogle Scholar
  19. [19]
    W. Taylor and M. Van Raamsdonk, Multiple D0-branes in weakly curved backgrounds, Nucl. Phys. B 558 (1999) 63 [hep-th/9904095] [INSPIRE].CrossRefADSGoogle Scholar
  20. [20]
    T. Yoneya, Generalized conformal symmetry and oblique AdS/CFT correspondence for matrix theory, Class. Quant. Grav. 17 (2000) 1307 [hep-th/9908153] [INSPIRE].CrossRefzbMATHADSMathSciNetGoogle Scholar
  21. [21]
    P. Yi, Witten index and threshold bound states of D-branes, Nucl. Phys. B 505 (1997) 307 [hep-th/9704098] [INSPIRE].CrossRefADSGoogle Scholar
  22. [22]
    S. Sethi and M. Stern, D-brane bound states redux, Commun. Math. Phys. 194 (1998) 675 [hep-th/9705046] [INSPIRE].CrossRefzbMATHADSMathSciNetGoogle Scholar
  23. [23]
    G.W. Moore, N. Nekrasov and S. Shatashvili, D-particle bound states and generalized instantons, Commun. Math. Phys. 209 (2000) 77 [hep-th/9803265] [INSPIRE].CrossRefzbMATHADSMathSciNetGoogle Scholar
  24. [24]
    M. Asano, Y. Sekino and T. Yoneya, PP wave holography for Dp-brane backgrounds, Nucl. Phys. B 678 (2004) 197 [hep-th/0308024] [INSPIRE].CrossRefADSMathSciNetGoogle Scholar
  25. [25]
    M. Asano and Y. Sekino, Large-N limit of SYM theories with 16 supercharges from superstrings on Dp-brane backgrounds, Nucl. Phys. B 705 (2005) 33 [hep-th/0405203] [INSPIRE].CrossRefADSMathSciNetGoogle Scholar
  26. [26]
    M. Asano, Stringy effect of the holographic correspondence for Dp-brane backgrounds, JHEP 12 (2004) 029 [hep-th/0408030] [INSPIRE].CrossRefADSMathSciNetGoogle Scholar
  27. [27]
    M. Hanada, J. Nishimura and S. Takeuchi, Non-lattice simulation for supersymmetric gauge theories in one dimension, Phys. Rev. Lett. 99 (2007) 161602 [arXiv:0706.1647] [INSPIRE].CrossRefADSGoogle Scholar
  28. [28]
    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].CrossRefADSGoogle Scholar
  29. [29]
    M. Hanada, Y. Hyakutake, J. Nishimura and S. Takeuchi, Higher derivative corrections to black hole thermodynamics from supersymmetric matrix quantum mechanics, Phys. Rev. Lett. 102 (2009) 191602 [arXiv:0811.3102] [INSPIRE].CrossRefADSGoogle Scholar
  30. [30]
    M. Hanada, A. Miwa, J. Nishimura and S. Takeuchi, Schwarzschild radius from Monte Carlo calculation of the Wilson loop in supersymmetric matrix quantum mechanics, Phys. Rev. Lett. 102 (2009) 181602 [arXiv:0811.2081] [INSPIRE].CrossRefADSGoogle Scholar
  31. [31]
    S. Catterall and T. Wiseman, Towards lattice simulation of the gauge theory duals to black holes and hot strings, JHEP 12 (2007) 104 [arXiv:0706.3518] [INSPIRE].CrossRefADSMathSciNetGoogle Scholar
  32. [32]
    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].ADSMathSciNetGoogle Scholar
  33. [33]
    S. Catterall and T. Wiseman, Extracting black hole physics from the lattice, JHEP 04 (2010) 077 [arXiv:0909.4947] [INSPIRE].CrossRefADSGoogle Scholar
  34. [34]
    A. Smilga, Comments on thermodynamics of supersymmetric matrix models, Nucl. Phys. B 818 (2009) 101 [arXiv:0812.4753] [INSPIRE].CrossRefADSMathSciNetGoogle Scholar
  35. [35]
    M. Hanada, S. Matsuura, J. Nishimura and D. Robles-Llana, Nonperturbative studies of supersymmetric matrix quantum mechanics with 4 and 8 supercharges at finite temperature,JHEP 02 (2011) 060 [arXiv:1012.2913] [INSPIRE].CrossRefADSMathSciNetGoogle Scholar
  36. [36]
    M. Campostrini and J. Wosiek, High precision study of the structure of D = 4 supersymmetric Yang-Mills quantum mechanics, Nucl. Phys. B 703 (2004) 454 [hep-th/0407021] [INSPIRE].CrossRefADSMathSciNetGoogle Scholar
  37. [37]
    J. Hiller, O. Lunin, S. Pinsky and U. Trittmann, Towards a SDLCQ test of the Maldacena conjecture, Phys. Lett. B 482 (2000) 409 [hep-th/0003249] [INSPIRE].ADSMathSciNetGoogle Scholar
  38. [38]
    J.R. Hiller, S.S. Pinsky, N. Salwen and U. Trittmann, Direct evidence for the Maldacena conjecture for \( \mathcal{N} \) = (8, 8) super Yang-Mills theory in 1 + 1 dimensions, Phys. Lett. B 624 (2005) 105 [hep-th/0506225] [INSPIRE].ADSMathSciNetGoogle Scholar
  39. [39]
    M. Hanada, J. Nishimura, Y. Sekino and T. Yoneya, Monte Carlo studies of matrix theory correlation functions, Phys. Rev. Lett. 104 (2010) 151601 [arXiv:0911.1623] [INSPIRE].CrossRefADSGoogle Scholar
  40. [40]
    T. Yoneya, String theory and space-time uncertainty principle, Prog. Theor. Phys. 103 (2000) 1081 [hep-th/0004074] [INSPIRE].CrossRefADSMathSciNetGoogle Scholar
  41. [41]
    G.T. Horowitz and A. Strominger, Black strings and p-branes, Nucl. Phys. B 360 (1991) 197 [INSPIRE].CrossRefADSMathSciNetGoogle Scholar
  42. [42]
    G. Gibbons and K. Maeda, Black holes and membranes in higher dimensional theories with dilaton fields, Nucl. Phys. B 298 (1988) 741 [INSPIRE].CrossRefADSMathSciNetGoogle Scholar
  43. [43]
    T. Azeyanagi, M. Hanada, H. Kawai and Y. Matsuo, Worldsheet analysis of gauge/gravity dualities, Nucl. Phys. B 816 (2009) 278 [arXiv:0812.1453] [INSPIRE].CrossRefADSMathSciNetGoogle Scholar
  44. [44]
    I. Kanitscheider, K. Skenderis and M. Taylor, Precision holography for non-conformal branes, JHEP 09 (2008) 094 [arXiv:0807.3324] [INSPIRE].CrossRefADSMathSciNetGoogle Scholar
  45. [45]
    D.E. Berenstein, J.M. Maldacena and H.S. Nastase, Strings in flat space and pp waves from \( \mathcal{N} \) =4 super Yang-Mills, JHEP 04 (2002) 013 [hep-th/0202021] [INSPIRE].CrossRefADSMathSciNetGoogle Scholar
  46. [46]
    S. Dobashi, H. Shimada and T. Yoneya, Holographic reformulation of string theory on AdS 5 × S 5 background in the pp wave limit, Nucl. Phys. B 665 (2003) 94 [hep-th/0209251] [INSPIRE].CrossRefADSMathSciNetGoogle Scholar
  47. [47]
    T. Yoneya, Holography in the large J limit of AdS/CFT correspondence and its applications, Prog. Theor. Phys. Suppl. 164 (2007) 82 [hep-th/0607046] [INSPIRE].CrossRefADSMathSciNetGoogle Scholar
  48. [48]
    S. Dobashi and T. Yoneya, Resolving the holography in the plane-wave limit of AdS/CFT correspondence, Nucl. Phys. B 711 (2005) 3 [hep-th/0406225] [INSPIRE].ADSMathSciNetGoogle Scholar
  49. [49]
    A. Miwa and T. Yoneya, Holography of Wilson-loop expectation values with local operator insertions, JHEP 12 (2006) 060 [hep-th/0609007] [INSPIRE].CrossRefADSMathSciNetGoogle Scholar
  50. [50]
    A. Tsuji, Holography of Wilson loop correlator and spinning strings, Prog. Theor. Phys. 117 (2007) 557 [hep-th/0606030] [INSPIRE].CrossRefzbMATHADSMathSciNetGoogle Scholar
  51. [51]
    S. Catterall and S. Karamov, Testing a Fourier accelerated hybrid Monte Carlo algorithm, Phys. Lett. B 528 (2002) 301 [hep-lat/0112025] [INSPIRE].ADSGoogle Scholar
  52. [52]
    M. Clark and A. Kennedy, The RHMC algorithm for two flavors of dynamical staggered fermions, Nucl. Phys. Proc. Suppl. 129 (2004) 850 [hep-lat/0309084] [INSPIRE].CrossRefADSGoogle Scholar
  53. [53]
    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].CrossRefADSGoogle Scholar
  54. [54]
    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].ADSMathSciNetGoogle Scholar
  55. [55]
    D. Berenstein, Large-N BPS states and emergent quantum gravity, JHEP 01 (2006) 125 [hep-th/0507203] [INSPIRE].CrossRefADSMathSciNetGoogle Scholar
  56. [56]
    J. Nishimura, Non-lattice simulation of supersymmetric gauge theories as a probe to quantum black holes and strings, PoS LAT2009 (2009) 016 [arXiv:0912.0327] [INSPIRE].
  57. [57]
    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 LATTICE2010 (2010) 253 [arXiv:1011.3904] [INSPIRE].
  58. [58]
    T. Ishii, G. Ishiki, S. Shimasaki and A. Tsuchiya, \( \mathcal{N} \)= 4 super Yang-Mills from the plane wave matrix model, Phys. Rev. D 78 (2008) 106001 [arXiv:0807.2352] [INSPIRE].ADSMathSciNetGoogle Scholar
  59. [59]
    G. Ishiki, S.-W. Kim, J. Nishimura and A. Tsuchiya, Deconfinement phase transition in \( \mathcal{N} \) =4 super Yang-Mills theory on R × S3 from supersymmetric matrix quantum mechanics, Phys. Rev. Lett. 102 (2009) 111601 [arXiv:0810.2884] [INSPIRE].CrossRefADSGoogle Scholar
  60. [60]
    G. Ishiki, S.-W. Kim, J. Nishimura and A. Tsuchiya, Testing a novel large-N reduction for \( \mathcal{N} \) =4 super Yang-Mills theory on R × S 3 , JHEP 09 (2009)029 [arXiv:0907.1488] [INSPIRE].CrossRefADSMathSciNetGoogle Scholar
  61. [61]
    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].CrossRefADSGoogle Scholar
  62. [62]
    M. Ünsal, Supersymmetric deformations of type IIB matrix model as matrix regularization of N =4 SYM,JHEP 04 (2006) 002 [hep-th/0510004] [INSPIRE].CrossRefADSGoogle Scholar
  63. [63]
    J.W. Elliott, J. Giedt and G.D. Moore, Lattice four-dimensional \( \mathcal{N} \)= 4 SYM is practical, Phys. Rev. D 78 (2008) 081701 [arXiv:0806.0013] [INSPIRE].ADSMathSciNetGoogle Scholar
  64. [64]
    S. Catterall, First results from simulations of supersymmetric lattices, JHEP 01 (2009) 040 [arXiv:0811.1203] [INSPIRE].CrossRefADSGoogle Scholar
  65. [65]
    J. Giedt, Progress in four-dimensional lattice supersymmetry, Int. J. Mod. Phys. A 24 (2009) 4045 [arXiv:0903.2443] [INSPIRE].ADSMathSciNetGoogle Scholar
  66. [66]
    S. Catterall, E. Dzienkowski, J. Giedt, A. Joseph and R. Wells, Perturbative renormalization of lattice \( \mathcal{N} \)= 4 super Yang-Mills theory, JHEP 04 (2011) 074 [arXiv:1102.1725] [INSPIRE].CrossRefADSMathSciNetGoogle Scholar
  67. [67]
    M. Hanada, S. Matsuura and F. Sugino, Two-dimensional lattice for four-dimensional \( \mathcal{N} \) = 4 supersymmetric Yang-Mills, Prog. Theor. Phys. 126 (2011) 597 [arXiv:1004.5513] [INSPIRE].CrossRefADSGoogle Scholar
  68. [68]
    M. Hanada, A proposal of a fine tuning free formulation of 4d \( \mathcal{N} \)= 4 super Yang-Mills, JHEP 11 (2010) 112 [arXiv:1009.0901] [INSPIRE].CrossRefADSGoogle Scholar
  69. [69]
    O. Aharony, J. Marsano, S. Minwalla and T. Wiseman, Black hole-black string phase transitions in thermal 1 + 1 dimensional supersymmetric Yang-Mills theory on a circle, Class. Quant. Grav. 21 (2004) 5169 [hep-th/0406210] [INSPIRE].CrossRefzbMATHADSMathSciNetGoogle Scholar
  70. [70]
    N. Kawahara, J. Nishimura and S. Takeuchi, Phase structure of matrix quantum mechanics at finite temperature, JHEP 10 (2007) 097 [arXiv:0706.3517] [INSPIRE].CrossRefADSMathSciNetGoogle Scholar
  71. [71]
    G. Mandal, M. Mahato and T. Morita, Phases of one dimensional large-N gauge theory in a 1/D expansion, JHEP 02 (2010) 034 [arXiv:0910.4526] [INSPIRE].CrossRefADSGoogle Scholar
  72. [72]
    I. Kanamori, H. Suzuki and F. Sugino, Euclidean lattice simulation for dynamical supersymmetry breaking, Phys. Rev. D 77 (2008) 091502 [arXiv:0711.2099] [INSPIRE].ADSGoogle Scholar
  73. [73]
    I. Kanamori, F. Sugino and H. Suzuki, Observing dynamical supersymmetry breaking with Euclidean lattice simulations, Prog. Theor. Phys. 119 (2008) 797 [arXiv:0711.2132] [INSPIRE].CrossRefzbMATHADSGoogle Scholar
  74. [74]
    I. Kanamori and H. Suzuki, Restoration of supersymmetry on the lattice: two-dimensional \( \mathcal{N} \)= (2,2) supersymmetric Yang-Mills theory, Nucl. Phys. B 811 (2009) 420 [arXiv:0809.2856] [INSPIRE].CrossRefADSMathSciNetGoogle Scholar
  75. [75]
    I. Kanamori and H. Suzuki, Some physics of the two-dimensional \( \mathcal{N} \)= (2, 2) supersymmetric Yang-Mills theory: lattice Monte Carlo study, Phys. Lett. B 672 (2009) 307 [arXiv:0811.2851] [INSPIRE].ADSMathSciNetGoogle Scholar
  76. [76]
    M. Hanada and I. Kanamori, Lattice study of two-dimensional \( \mathcal{N} \)= (2, 2) super Yang-Mills at large N , Phys. Rev. D 80 (2009) 065014 [arXiv:0907.4966] [INSPIRE].ADSGoogle Scholar
  77. [77]
    M. Hanada and I. Kanamori, Absence of sign problem in two-dimensional \( \mathcal{N} \)= (2, 2) super Yang-Mills on lattice, JHEP 01 (2011) 058 [arXiv:1010.2948] [INSPIRE].CrossRefADSMathSciNetGoogle Scholar
  78. [78]
    S. Catterall, A. Joseph and T. Wiseman, Thermal phases of D1-branes on a circle from lattice super Yang-Mills, JHEP 12 (2010) 022 [arXiv:1008.4964] [INSPIRE].CrossRefADSMathSciNetGoogle Scholar
  79. [79]
    R. Dijkgraaf, E.P. Verlinde and H.L. Verlinde, Matrix string theory, Nucl. Phys. B 500 (1997) 43 [hep-th/9703030] [INSPIRE].CrossRefADSMathSciNetGoogle Scholar
  80. [80]
    Y. Sekino and T. Yoneya, From supermembrane to matrix string, Nucl. Phys. B 619 (2001) 22 [hep-th/0108176] [INSPIRE].CrossRefADSMathSciNetGoogle Scholar
  81. [81]
    S. Duane, A. Kennedy, B. Pendleton and D. Roweth, Hybrid Monte Carlo, Phys. Lett. B 195 (1987) 216 [INSPIRE].ADSGoogle Scholar
  82. [82]
    J. Ambjørn, K. Anagnostopoulos, W. Bietenholz, T. Hotta and J. Nishimura, Large-N dynamics of dimensionally reduced 4d SU(N ) super Yang-Mills theory, JHEP 07 (2000) 013 [hep-th/0003208] [INSPIRE].CrossRefADSGoogle Scholar
  83. [83]
    J. Ambjørn, K. Anagnostopoulos, W. Bietenholz, T. Hotta and J. Nishimura, Monte Carlo studies of the IIB matrix model at large N , JHEP 07 (2000) 011 [hep-th/0005147] [INSPIRE].CrossRefADSGoogle Scholar
  84. [84]
    M.A. Clark and A.D. Kennedy, http://www.ph.ed.ac.uk/mike/remez,2005.
  85. [85]
    B. Jegerlehner, Krylov space solvers for shifted linear systems, hep-lat/9612014 [INSPIRE].
  86. [86]
    K. Anagnostopoulos and J. Nishimura, New approach to the complex action problem and its application to a nonperturbative study of superstring theory, Phys. Rev. D 66 (2002) 106008 [hep-th/0108041] [INSPIRE].ADSMathSciNetGoogle Scholar
  87. [87]
    J. Ambjørn, K. Anagnostopoulos, J. Nishimura and J. Verbaarschot, The factorization method for systems with a complex action: a test in random matrix theory for finite density QCD, JHEP 10 (2002) 062 [hep-lat/0208025] [INSPIRE].CrossRefADSGoogle Scholar
  88. [88]
    K.N. Anagnostopoulos, T. Azuma and J. Nishimura, A general approach to the sign problem: the factorization method with multiple observables, Phys. Rev. D 83 (2011) 054504 [arXiv:1009.4504] [INSPIRE].ADSGoogle Scholar
  89. [89]
    K.N. Anagnostopoulos, T. Azuma and J. Nishimura, A practical solution to the sign problem in a matrix model for dynamical compactification, JHEP 10 (2011) 126 [arXiv:1108.1534] [INSPIRE].CrossRefADSGoogle Scholar

Copyright information

© SISSA, Trieste, Italy 2011

Authors and Affiliations

  • Masanori Hanada
    • 1
    Email author
  • Jun Nishimura
    • 2
    • 3
  • Yasuhiro Sekino
    • 2
  • Tamiaki Yoneya
    • 4
    • 5
  1. 1.Department of PhysicsUniversity of WashingtonSeattleU.S.A.
  2. 2.KEK Theory CenterHigh Energy Accelerator Research Organization (KEK)TsukubaJapan
  3. 3.Department of Particle and Nuclear Physics, School of High Energy Accelerator ScienceGraduate University for Advanced Studies (SOKENDAI)TsukubaJapan
  4. 4.School of Graduate StudiesThe Open University of JapanMihama-kuJapan
  5. 5.Institute of PhysicsUniversity of TokyoKomabaJapan

Personalised recommendations