Type IIA Pati-Salam flux vacua

被引:26
|
作者
Chen, CM
Li, TJ [1 ]
Nanopoulos, DV
机构
[1] Rutgers State Univ, Dept Phys & Astron, Piscataway, NJ 08854 USA
[2] Texas A&M Univ, George P & Cynthia W Mitchell Inst Fundamental Ph, College Stn, TX 77843 USA
[3] Chinese Acad Sci, Inst Theoret Phys, Beijing 100080, Peoples R China
[4] Houston Adv Res Ctr, Astroparticle Phys Grp, The Woodlands, TX 77381 USA
[5] Acad Athens, Div Nat Sci, Athens 10679, Greece
关键词
D O I
10.1016/j.nuclphysb.2006.01.039
中图分类号
O412 [相对论、场论]; O572.2 [粒子物理学];
学科分类号
摘要
We show that for supersymmetric AdS vacua on type IIA orientifolds with flux compactifications, the RR tadpole cancellation conditions can be completely relaxed, and then the four-dimensional N = I supersymmetry conditions are the main constraints on consistent intersecting D6-brane model building. We construct two kinds of three-family Pati-Salam models. In the first kind of models, the suitable three-family SM fermion masses and mixings can be generated at the stringy tree level, and then the rank one problem for the SM fermion Yukawa matrices can be solved. In the second kind of models, only the third family of the SM fermions can obtain masses at tree level. In these models, the complex structure parameters can be determined by supersymmetric D6-brane configurations, and all the moduli may be stabilized. The initial gauge symmetries U(4)(C) x U(2)(L) x U(2)(R) and U(4)(C) x USp(2)(L) x U(2)(R) can be broken down to the SU(3)(C) x SU(2)(L) X U(1)(B-L) X U(1)(I3R) due to the Green-Schwarz mechanism and D6-brane splittings, and further down to the SM gauge symmetry around the string scale via the supersymmetry preserving Higgs mechanism. Comparing to the previous model building, we have less bidoublet Higgs fields. However, there generically exist some exotic particles. (c) 2006 Elsevier B.V. All rights reserved.
引用
收藏
页码:79 / 104
页数:26
相关论文
共 50 条
  • [1] The "landscape" of Pati-Salam heterotic superstring vacua
    Rizos, J.
    [J]. FORTSCHRITTE DER PHYSIK-PROGRESS OF PHYSICS, 2010, 58 (7-9): : 758 - 762
  • [2] Phenomenological analysis of D-brane Pati-Salam vacua
    Anastasopoulos, P.
    Leontaris, G. K.
    Vlachos, N. D.
    [J]. JOURNAL OF HIGH ENERGY PHYSICS, 2010, (05):
  • [3] Phenomenological analysis of D-brane Pati-Salam vacua
    P. Anastasopoulos
    G. K. Leontaris
    N. D. Vlachos
    [J]. Journal of High Energy Physics, 2010
  • [4] Pati-Salam axion
    Di Luzio, Luca
    [J]. JOURNAL OF HIGH ENERGY PHYSICS, 2020, 2020 (07)
  • [5] Pati-Salam axion
    Luca Di Luzio
    [J]. Journal of High Energy Physics, 2020
  • [6] A to Z of Flavour with Pati-Salam
    Stephen F. King
    [J]. Journal of High Energy Physics, 2014
  • [7] HOW UNIQUE IS THE PATI-SALAM TYPE GRAND UNIFICATION
    TOSA, Y
    [J]. PHYSICAL REVIEW D, 1982, 25 (04) : 1150 - 1153
  • [8] IMPROVED PATI-SALAM MODELS
    SCHORR, A
    [J]. PHYSICAL REVIEW D, 1978, 18 (03): : 863 - 878
  • [9] A to Z of Flavour with Pati-Salam
    King, Stephen F.
    [J]. JOURNAL OF HIGH ENERGY PHYSICS, 2014, (08):
  • [10] GENERALIZATION OF PATI-SALAM MODEL
    ELIAS, V
    SWIFT, AR
    [J]. PHYSICAL REVIEW D, 1976, 13 (07): : 2083 - 2090