Abstract:Abstract:We propose new backgrounds of extra dimensions to lead to four-dimensional chiral models with three generations of matter fermions, that is T 2 /Z N twisted orbifolds with magnetic fluxes. We consider gauge theory on six-dimensional space-time, which contains the T 2 /Z N orbifold with magnetic flux, Scherk-Schwarz phases and Wilson line phases. We classify all the possible Scherk-Schwarz and Wilson line phases on T 2 /Z N orbifolds with magnetic fluxes. The behavior of zero modes is studied. We deriv… Show more
“…This case is interesting because the hierarchical structure of the Yukawa coupling constants can be realized by the wave function localization [24,25], and the generation structure can also be obtained by a background magnetic flux [22]. In the following, we focus on the quark sector, but a similar argument is also applicable to the lepton sector.…”
Section: Matter Fieldmentioning
confidence: 99%
“…In fact, when (N, n P , m ω ) = (3, 1, 0), the fermionic zero-modes from each 6D Dirac fermion contain 22) and when (N, n P , m ω ) = (3, 2, 2), they contain…”
Section: Jhep08(2014)175mentioning
confidence: 99%
“…The number of the zero-modes j max is determined by the magnetic flux [22]. The zero-mode functions f (j)µ χ 6 (z) are determined so that (5.3) satisfies the first two conditions in (5.2).…”
Abstract:We investigate the gauge-Higgs unification models compactified on T 2 /Z N that have the custodial symmetry. We select possible gauge groups, orbifolds and representations of the matter fermions that are consistent with the custodial symmetry, by means of the group theoretical analysis. The best candidate we found is 6D SU(3) C × U(4) gauge theory on T 2 /Z 3 and the third generation quarks are embedded into bulk fermions that are the symmetric traceless rank-2 tensor of SO(6).
“…This case is interesting because the hierarchical structure of the Yukawa coupling constants can be realized by the wave function localization [24,25], and the generation structure can also be obtained by a background magnetic flux [22]. In the following, we focus on the quark sector, but a similar argument is also applicable to the lepton sector.…”
Section: Matter Fieldmentioning
confidence: 99%
“…In fact, when (N, n P , m ω ) = (3, 1, 0), the fermionic zero-modes from each 6D Dirac fermion contain 22) and when (N, n P , m ω ) = (3, 2, 2), they contain…”
Section: Jhep08(2014)175mentioning
confidence: 99%
“…The number of the zero-modes j max is determined by the magnetic flux [22]. The zero-mode functions f (j)µ χ 6 (z) are determined so that (5.3) satisfies the first two conditions in (5.2).…”
Abstract:We investigate the gauge-Higgs unification models compactified on T 2 /Z N that have the custodial symmetry. We select possible gauge groups, orbifolds and representations of the matter fermions that are consistent with the custodial symmetry, by means of the group theoretical analysis. The best candidate we found is 6D SU(3) C × U(4) gauge theory on T 2 /Z 3 and the third generation quarks are embedded into bulk fermions that are the symmetric traceless rank-2 tensor of SO(6).
“…These degrees of freedom are equivalent to each other [28]. Hence, we restrict ourselves to Scherk-Schwarz phases.…”
Section: A Magnetized Torus Modelsmentioning
confidence: 99%
“…Zero-mode wave functions were studied by numerical studies [28] and the corresponding states were studied by operator analysis in quantum mechanism [29]. By use of those results, model building and fermion mass matrices were also studied [30][31][32].…”
We study T 2 =Z N orbifold models with magnetic fluxes. We propose a systematic way to analyze the number of zero-modes and their wave functions by use of modular transformation. Our results are consistent with the previous results, and our approach is more direct and analytical than the previous ones. The index theorem implies that the zero-mode number of the Dirac operator on T 2 is equal to the index M, which corresponds to the magnetic flux in a certain unit. Our results show that the zero-mode number of the Dirac operator on T 2 =Z N is equal to ⌊M=N⌋ þ 1 except one case on the T 2 =Z 3 orbifold.
We discuss the flavor structure in resolution of magnetized T 2 /Z 2 orbifold models. The flavor structure of Yukawa couplings among chiral zero-modes is sensitive to radii of the resolved fixed points of T 2 /Z 2 orbifold. We show in concrete models that the realistic mass hierarchy and mixing angles of the quark sector can be realized at certain values of blow-up radii, where the number of parameters in the blow-up model can be smaller than toroidal orbifold one.
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