227 research outputs found

    Realistic Type IIB Supersymmetric Minkowski Flux Vacua

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    We show that there exist supersymmetric Minkowski vacua on Type IIB toroidal orientifold with general flux compactifications where the RR tadpole cancellation conditions can be relaxed elegantly. Then we present a realistic Pati-Salam like model. At the string scale, the gauge symmetry can be broken down to the Standard Model (SM) gauge symmetry, the gauge coupling unification can be achieved naturally, and all the extra chiral exotic particles can be decoupled so that we have the supersymmetric SMs with/without SM singlet(s) below the string scale. The observed SM fermion masses and mixings can also be obtained. In addition, the unified gauge coupling, the dilaton, the complex structure moduli, the real parts of the K\"ahler moduli and the sum of the imaginary parts of the K\"ahler moduli can be determined as functions of the four-dimensional dilaton and fluxes, and can be estimated as well.Comment: RevTex4, 4 pages, 3 table

    The Minimal GUT with Inflaton and Dark Matter Unification

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    Giving up the solutions to the fine-tuning problems, we propose the non-supersymmetric flipped SU(5)Ă—U(1)XSU(5)\times U(1)_X model based on the minimal particle content principle, which can be constructed from the four-dimensional SO(10)SO(10) models, five-dimensional orbifold SO(10)SO(10) models, and local F-theory SO(10)SO(10) models. To achieve gauge coupling unification, we introduce one pair of vector-like fermions, which form complete SU(5)Ă—U(1)XSU(5)\times U(1)_X representation. Proton lifetime is around 5Ă—10355\times 10^{35} years, neutrino masses and mixing can be explained via seesaw mechanism, baryon asymmetry can be generated via leptogenesis, and vacuum stability problem can be solved as well. In particular, we propose that inflaton and dark matter particle can be unified to a real scalar field with Z2Z_2 symmetry, which is not an axion and does not have the non-minimal coupling to gravity. Such kind of scenarios can be applied to the generic scalar dark matter models. Also, we find that the vector-like particle corrections to the Bs0B_s^0 masses can be about 6.6%, while their corrections to the K0K^0 and Bd0B_d^0 masses are negligible.Comment: 5 pages, 4 figures;V2: published versio

    Yukawa Corrections from Four-Point Functions in Intersecting D6-Brane Models

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    We discuss corrections to the Yukawa matrices of the Standard Model (SM) fermions in intersecting D-brane models due to four-point interactions. Recently, an intersecting D-brane model has been found where it is possible to obtain correct masses and mixings for all quarks as well as the tau lepton. However, the masses for the first two charged leptons come close to the right values but are not quite correct. Since the electron and muon are quite light, it is likely that there are additional corrections to their masses which cannot be neglected. With this in mind, we consider contributions to the SM fermion mass matrices from four-point interactions. In an explicit model, we show that it is indeed possible to obtain the SM fermion masses and mixings which are a better match to those resulting from experimental data extrapolated at the unification scale when these corrections are included. These corrections may have broader application to other models.Comment: 24 pages, 4 figure

    A Realistic World from Intersecting D6-Branes

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    We briefly describe a three-family intersecting D6-brane model in Type IIA theory on the T^6/(Z_2 x Z_2) orientifold with a realistic phenomenology. In this model, the gauge symmetry can be broken down to the Standard Model (SM) gauge symmetry close to the string scale, and the gauge coupling unification can be achieved. We calculate the supersymmetry breaking soft terms, and the corresponding low energy supersymmetric particle spectrum, which may be tested at the Large Hadron Collider (LHC). The observed dark matter density may also be generated. Finally, we can explain the SM quark masses and CKM mixings, and the tau lepton mass. The neutrino masses and mixings may be generated via the seesaw mechanism as well.Comment: RevTex4, 4 pages, 4 table
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