Advertisement

Realizing three generations of the Standard Model fermions in the type IIB matrix model

  • Hajime Aoki
  • Jun NishimuraEmail author
  • Asato Tsuchiya
Open Access
Article

Abstract

We discuss how the Standard Model particles appear from the type IIB matrix model, which is considered to be a nonperturbative formulation of superstring theory. In particular, we are concerned with a constructive definition of the theory, in which we start with finite-N matrices and take the large-N limit afterwards. In that case, it was pointed out recently that realizing chiral fermions in the model is more difficult than it had been thought from formal arguments at N = ∞ and that introduction of a matrix version of the warp factor is necessary. Based on this new insight, we show that two generations of the Standard Model fermions can be realized by considering a rather generic configuration of fuzzy S2 and fuzzy S2 × S2 in the extra dimensions. We also show that three generations can be obtained by squashing one of the S2’s that appear in the configuration. Chiral fermions appear at the intersections of the fuzzy manifolds with nontrivial Yukawa couplings to the Higgs field, which can be calculated from the overlap of their wave functions.

Keywords

Matrix Models Superstring Vacua 

Notes

Open Access

This article is distributed under the terms of the Creative Commons Attribution License (CC-BY 4.0), which permits any use, distribution and reproduction in any medium, provided the original author(s) and source are credited.

References

  1. [1]
    N. Ishibashi, H. Kawai, Y. Kitazawa and A. Tsuchiya, A large-N reduced model as superstring, Nucl. Phys. B 498 (1997) 467 [hep-th/9612115] [INSPIRE].ADSMathSciNetCrossRefzbMATHGoogle Scholar
  2. [2]
    W. Krauth, H. Nicolai and M. Staudacher, Monte Carlo approach to M-theory, Phys. Lett. B 431 (1998) 31 [hep-th/9803117] [INSPIRE].ADSMathSciNetCrossRefGoogle Scholar
  3. [3]
    P. Austing and J.F. Wheater, Convergent Yang-Mills matrix theories, JHEP 04 (2001) 019 [hep-th/0103159] [INSPIRE].ADSMathSciNetCrossRefGoogle Scholar
  4. [4]
    J. Nishimura, T. Okubo and F. Sugino, Systematic study of the SO(10) symmetry breaking vacua in the matrix model for type IIB superstrings, JHEP 10 (2011) 135 [arXiv:1108.1293] [INSPIRE].ADSMathSciNetCrossRefzbMATHGoogle Scholar
  5. [5]
    K.N. Anagnostopoulos, T. Azuma and J. Nishimura, Monte Carlo studies of the spontaneous rotational symmetry breaking in dimensionally reduced super Yang-Mills models, JHEP 11 (2013) 009 [arXiv:1306.6135] [INSPIRE].ADSCrossRefzbMATHGoogle Scholar
  6. [6]
    S.-W. Kim, J. Nishimura and A. Tsuchiya, Expanding (3+1)-dimensional universe from a Lorentzian matrix model for superstring theory in (9+1)-dimensions, Phys. Rev. Lett. 108 (2012) 011601 [arXiv:1108.1540] [INSPIRE].ADSCrossRefGoogle Scholar
  7. [7]
    H. Aoki, S. Iso and T. Suyama, Orbifold matrix model, Nucl. Phys. B 634 (2002) 71 [hep-th/0203277] [INSPIRE].ADSMathSciNetCrossRefzbMATHGoogle Scholar
  8. [8]
    A. Chatzistavrakidis, H. Steinacker and G. Zoupanos, Orbifolds, fuzzy spheres and chiral fermions, JHEP 05 (2010) 100 [arXiv:1002.2606] [INSPIRE].ADSMathSciNetCrossRefzbMATHGoogle Scholar
  9. [9]
    A. Chatzistavrakidis, H. Steinacker and G. Zoupanos, Orbifold matrix models and fuzzy extra dimensions, PoS CORFU2011 (2011) 047 [arXiv:1204.6498] [INSPIRE].
  10. [10]
    H. Aoki, Chiral fermions and the standard model from the matrix model compactified on a torus, Prog. Theor. Phys. 125 (2011) 521 [arXiv:1011.1015] [INSPIRE].ADSCrossRefzbMATHGoogle Scholar
  11. [11]
    H. Abe, T. Kobayashi, H. Ohki, A. Oikawa and K. Sumita, Phenomenological aspects of 10D SYM theory with magnetized extra dimensions, Nucl. Phys. B 870 (2013) 30 [arXiv:1211.4317] [INSPIRE].ADSMathSciNetCrossRefzbMATHGoogle Scholar
  12. [12]
    H. Abe, T. Kobayashi, H. Ohki, K. Sumita and Y. Tatsuta, Flavor landscape of 10D SYM theory with magnetized extra dimensions, JHEP 04 (2014) 007 [arXiv:1307.1831] [INSPIRE].ADSCrossRefGoogle Scholar
  13. [13]
    H. Aoki, Probability of the Standard Model appearance from a matrix model, Phys. Rev. D 87 (2013) 046002 [arXiv:1209.4514] [INSPIRE].ADSGoogle Scholar
  14. [14]
    H. Aoki, Probability distribution over some phenomenological models in the matrix model compactified on a torus, PTEP 2013 (2013) 0903B04 [arXiv:1303.3982] [INSPIRE].Google Scholar
  15. [15]
    A. Chatzistavrakidis, H. Steinacker and G. Zoupanos, Intersecting branes and a standard model realization in matrix models, JHEP 09 (2011) 115 [arXiv:1107.0265] [INSPIRE].ADSMathSciNetCrossRefzbMATHGoogle Scholar
  16. [16]
    M. Berkooz, M.R. Douglas and R.G. Leigh, Branes intersecting at angles, Nucl. Phys. B 480 (1996) 265 [hep-th/9606139] [INSPIRE].ADSMathSciNetCrossRefzbMATHGoogle Scholar
  17. [17]
    I. Antoniadis, E. Kiritsis and T.N. Tomaras, A D-brane alternative to unification, Phys. Lett. B 486 (2000) 186 [hep-ph/0004214] [INSPIRE].ADSMathSciNetCrossRefzbMATHGoogle Scholar
  18. [18]
    G. Aldazabal, L.E. Ibáñez, F. Quevedo and A.M. Uranga, D-branes at singularities: a bottom up approach to the string embedding of the standard model, JHEP 08 (2000) 002 [hep-th/0005067] [INSPIRE].ADSMathSciNetCrossRefzbMATHGoogle Scholar
  19. [19]
    R. Blumenhagen, L. Görlich, B. Körs and D. Lüst, Noncommutative compactifications of type-I strings on tori with magnetic background flux, JHEP 10 (2000) 006 [hep-th/0007024] [INSPIRE].ADSMathSciNetCrossRefzbMATHGoogle Scholar
  20. [20]
    L.E. Ibáñez, F. Marchesano and R. Rabadán, Getting just the standard model at intersecting branes, JHEP 11 (2001) 002 [hep-th/0105155] [INSPIRE].MathSciNetGoogle Scholar
  21. [21]
    R. Blumenhagen, B. Körs, D. Lüst and T. Ott, The standard model from stable intersecting brane world orbifolds, Nucl. Phys. B 616 (2001) 3 [hep-th/0107138] [INSPIRE].ADSMathSciNetCrossRefzbMATHGoogle Scholar
  22. [22]
    M. Cvetič, G. Shiu and A.M. Uranga, Three family supersymmetric standard - like models from intersecting brane worlds, Phys. Rev. Lett. 87 (2001) 201801 [hep-th/0107143] [INSPIRE].ADSMathSciNetCrossRefGoogle Scholar
  23. [23]
    M. Cvetič, G. Shiu and A.M. Uranga, Chiral four-dimensional N = 1 supersymmetric type 2A orientifolds from intersecting D6 branes, Nucl. Phys. B 615 (2001) 3 [hep-th/0107166] [INSPIRE].ADSCrossRefzbMATHGoogle Scholar
  24. [24]
    D. Cremades, L.E. Ibáñez and F. Marchesano, Standard model at intersecting D5-branes: Lowering the string scale, Nucl. Phys. B 643 (2002) 93 [hep-th/0205074] [INSPIRE].ADSMathSciNetCrossRefzbMATHGoogle Scholar
  25. [25]
    C. Kokorelis, New standard model vacua from intersecting branes, JHEP 09 (2002) 029 [hep-th/0205147] [INSPIRE].ADSMathSciNetCrossRefzbMATHGoogle Scholar
  26. [26]
    C. Kokorelis, Exact standard model structures from intersecting D5-branes, Nucl. Phys. B 677 (2004) 115 [hep-th/0207234] [INSPIRE].ADSMathSciNetCrossRefzbMATHGoogle Scholar
  27. [27]
    H. Steinacker and J. Zahn, An index for intersecting branes in matrix models, SIGMA 9 (2013) 067 [arXiv:1309.0650] [INSPIRE].MathSciNetzbMATHGoogle Scholar
  28. [28]
    J. Nishimura and A. Tsuchiya, Realizing chiral fermions in the type IIB matrix model at finite N, JHEP 12 (2013) 002 [arXiv:1305.5547] [INSPIRE].ADSCrossRefGoogle Scholar
  29. [29]
    R.C. Myers, Dielectric branes, JHEP 12 (1999) 022 [hep-th/9910053] [INSPIRE].ADSMathSciNetCrossRefzbMATHGoogle Scholar
  30. [30]
    T. Imai, Y. Kitazawa, Y. Takayama and D. Tomino, Quantum corrections on fuzzy sphere, Nucl. Phys. B 665 (2003) 520 [hep-th/0303120] [INSPIRE].ADSMathSciNetCrossRefzbMATHGoogle Scholar
  31. [31]
    T. Imai, Y. Kitazawa, Y. Takayama and D. Tomino, Effective actions of matrix models on homogeneous spaces, Nucl. Phys. B 679 (2004) 143 [hep-th/0307007] [INSPIRE].ADSMathSciNetCrossRefzbMATHGoogle Scholar
  32. [32]
    H. Kaneko, Y. Kitazawa and D. Tomino, Stability of fuzzy S 2 × S 2 × S 2 in IIB type matrix models, Nucl. Phys. B 725 (2005) 93 [hep-th/0506033] [INSPIRE].ADSCrossRefzbMATHGoogle Scholar
  33. [33]
    H.C. Steinacker and J. Zahn, An extended standard model and its Higgs geometry from the matrix model, arXiv:1401.2020 [INSPIRE].
  34. [34]
    M. Fukuma, H. Kawai, Y. Kitazawa and A. Tsuchiya, String field theory from IIB matrix model, Nucl. Phys. B 510 (1998) 158 [hep-th/9705128] [INSPIRE].MathSciNetCrossRefzbMATHGoogle Scholar
  35. [35]
    H. Aoki, S. Iso, H. Kawai, Y. Kitazawa and T. Tada, Space-time structures from IIB matrix model, Prog. Theor. Phys. 99 (1998) 713 [hep-th/9802085] [INSPIRE].ADSMathSciNetCrossRefGoogle Scholar
  36. [36]
    S.-W. Kim, J. Nishimura and A. Tsuchiya, Expanding universe as a classical solution in the Lorentzian matrix model for nonperturbative superstring theory, Phys. Rev. D 86 (2012) 027901 [arXiv:1110.4803] [INSPIRE].ADSGoogle Scholar
  37. [37]
    S.-W. Kim, J. Nishimura and A. Tsuchiya, Late time behaviors of the expanding universe in the IIB matrix model, JHEP 10 (2012) 147 [arXiv:1208.0711] [INSPIRE].ADSCrossRefGoogle Scholar
  38. [38]
    J. Nishimura and A. Tsuchiya, Local field theory from the expanding universe at late times in the IIB matrix model, PTEP 2013 (2013) 043B03 [arXiv:1208.4910] [INSPIRE].
  39. [39]
    G.C. Branco et al., Theory and phenomenology of two-Higgs-doublet models, Phys. Rept. 516 (2012) 1 [arXiv:1106.0034] [INSPIRE].ADSCrossRefGoogle Scholar
  40. [40]
    N. Arkani-Hamed, S. Dimopoulos and G.R. Dvali, The hierarchy problem and new dimensions at a millimeter, Phys. Lett. B 429 (1998) 263 [hep-ph/9803315] [INSPIRE].
  41. [41]
    N.S. Manton, A new six-dimensional approach to the Weinberg-Salam model, Nucl. Phys. B 158 (1979) 141 [INSPIRE].ADSMathSciNetCrossRefGoogle Scholar
  42. [42]
    D.B. Fairlie, Higgsfields and the determination of the Weinberg angle, Phys. Lett. B 82 (1979) 97 [INSPIRE].ADSCrossRefGoogle Scholar
  43. [43]
    D.B. Fairlie, Two consistent calculations of the Weinberg angle, J. Phys. G 5 (1979) L55 [INSPIRE].ADSCrossRefGoogle Scholar
  44. [44]
    Y. Hosotani, Dynamical mass generation by compact extra dimensions, Phys. Lett. B 126 (1983) 309 [INSPIRE].ADSCrossRefGoogle Scholar
  45. [45]
    Y. Hosotani, Dynamical gauge symmetry breaking as the Casimir effectc, Phys. Lett. B 129 (1983) 193 [INSPIRE].ADSCrossRefGoogle Scholar
  46. [46]
    Y. Hosotani, Dynamics of nonintegrable phases and gauge symmetry breaking, Annals Phys. 190 (1989) 233 [INSPIRE].ADSMathSciNetCrossRefGoogle Scholar
  47. [47]
    H. Hatanaka, T. Inami and C.S. Lim, The gauge hierarchy problem and higher dimensional gauge theories, Mod. Phys. Lett. A 13 (1998) 2601 [hep-th/9805067] [INSPIRE].ADSCrossRefGoogle Scholar
  48. [48]
    S. Iso, Y. Kimura, K. Tanaka and K. Wakatsuki, Noncommutative gauge theory on fuzzy sphere from matrix model, Nucl. Phys. B 604 (2001) 121 [hep-th/0101102] [INSPIRE].ADSMathSciNetCrossRefzbMATHGoogle Scholar
  49. [49]
    D. Cremades, L.E. Ibáñez and F. Marchesano, Computing Yukawa couplings from magnetized extra dimensions, JHEP 05 (2004) 079 [hep-th/0404229] [INSPIRE].ADSCrossRefGoogle Scholar
  50. [50]
    Y. Ito, S.-W. Kim, J. Nishimura and A. Tsuchiya, Monte Carlo studies on the expanding behavior of the early universe in the Lorentzian type IIB matrix model, PoS(LATTICE2013)341 [arXiv:1311.5579] [INSPIRE].
  51. [51]
    Y. Ito, S.-W. Kim, Y. Koizuka, J. Nishimura and A. Tsuchiya, A renormalization group method for studying the early universe in the Lorentzian IIB matrix model, arXiv:1312.5415 [INSPIRE].

Copyright information

© The Author(s) 2014

Authors and Affiliations

  1. 1.Department of PhysicsSaga UniversitySagaJapan
  2. 2.Department of Particle and Nuclear PhysicsGraduate University for Advanced Studies (SOKENDAI)TsukubaJapan
  3. 3.KEK Theory Center, High Energy Accelerator Research OrganizationTsukubaJapan
  4. 4.Department of PhysicsShizuoka UniversitySuruga-kuJapan

Personalised recommendations