111 research outputs found

    CPCP violation in minimal supersymmetric standard model

    Full text link
    CPCP violating phenomena predicted by the minimal supersymmetric standard model are discussed in a case where the CPCP violating phases in SUSY sector are not suppressed. The electric dipole moments of the neutron and the electron are large, but can be smaller than their experimental upper bounds if the scalar quarks and leptons are heavier than a few TeV. TT violating asymmetries in the production processes of the different neutralino pair and the different chargino pair emerge at the tree level. They could be as large as of order 10−210^{-2} in unpolarized electron beam experiments and 10−110^{-1} in polarized electron beam experiments. In a pair production of the charginos of the same mass, the asymmetry emerges through the electric and the weak "electric" dipole moments of the charginos at the loop level, but its magnitude is at most of order 10−410^{-4}.Comment: 7 pages with 7 figures, TKU-HEP 94/02; IFM 2/94, LaTeX with Elsevir Science Publisher's style file, espcrc2.sty. (To appear in the proceedings of the Third KEK Topical Conference on CP Violation, November 1993) Figures are not included. The complete PostScript file can be obtained by anonymous ftp from ape.sp.u-tokai.ac.jp in the directr

    Decay Rate Asymmetry of Top Squark

    Get PDF
    We discuss a decay rate asymmetry of the top squark, which is induced by a new source of CP violation intrinsic in the supersymmetric standard model. Although new sources of CP violation in this model are severely constrained from the electric dipole moment of the neutron, an unsuppressed CP-violating phase can still coexist with a top squark whose mass is accessible by near-future colliders. Then the dominant decay mode of the top squark has a width different from its CP conjugate process. The magnitude of this CPCP asymmetry becomes of order 10−310^{-3}.Comment: 11 pages, 1 figur

    CP violation in minimal supersymmetric standard model

    Get PDF

    Effect on the electron EDM due to abelian gauginos in SUSY extra U(1) models

    Full text link
    The electric dipole moment of an electron (EDME) is investigated in the supersymmetric extra U(1) models. Neutralino sector is generally extended in these models and then the neutralino contribution will be important for the analysis of the EDME. Kinetic term mixings of abelian gauginos are taken into account in our analysis. Numerical results for the extra U(1) models show that the EDME can be affected by the extra U(1) in a certain range of soft supersymmetry breaking parameters even if the extra U(1) gauge boson is heavy. The EDME may be a clue to find an extended gauge structure in the supersymmetric models.Comment: 16 pages, latex, 3 figure

    Supersymmetric Extension of the Standard Model with Naturally Stable Proton

    Get PDF
    A new supersymmetric standard model based on N=1 supergravity is constructed, aiming at natural explanation for the proton stability without invoking an ad hoc discrete symmetry through R parity. The proton is protected from decay by an extra U(1) gauge symmetry. Particle contents are necessarily increased to be free from anomalies, making it possible to incorporate the superfields for right-handed neutrinos and an SU(2)-singlet Higgs boson. The vacuum expectation value of this Higgs boson, which induces spontaneous breakdown of the U(1) symmetry, yields large Majorana masses for the right-handed neutrinos, leading to small masses for the ordinary neutrinos. The linear coupling of SU(2)-doublet Higgs superfields, which is indispensable to the superpotential of the minimal supersymmetric standard model, is replaced by a trilinear coupling of the Higgs superfields, so that there is no mass parameter in the superpotential. The energy dependencies of the model parameters are studied, showing that gauge symmetry breaking is induced by radiative corrections. Certain ranges of the parameter values compatible with phenomena at the electroweak energy scale can be derived from universal values of masses-squared and trilinear coupling constants for scalar fields at a very high energy scale.Comment: 32 pages, Revtex, 7 figure

    A Supersymmetric Model with an Extra U(1) Gauge Symmetry

    Get PDF
    In the standard model the proton is protected from decay naturally by gauge symmetries, whereas in the ordinary minimal supersymmetric standard model an ad hoc discrete symmetry is imposed for the proton stability. We present a new supersymmetric model in which the proton decay is forbidden by an extra U(1) gauge symmetry. Particle contents are necessarily increased to be free from anomalies, incorporating right-handed neutrinos. Both Dirac and Majorana masses are generated for neutrinos, yielding non-vanishing but small masses. The superpotential consists only of trilinear couplings and the mass parameter Ό\mu of the minimal model is induced by spontaneous breaking of the U(1) symmetry.Comment: 10 pages, Revte

    CP violating asymmetries in single top quark production at the Tevatron p pbar collider

    Get PDF
    Analytic expressions for the angular distributions of the bb-quarks associated with single tt-quark production in ppˉ→W∗→tbˉ→bbˉWp \bar p \to W^* \to t \bar b \to b \bar b W and of the leptons from the subsequent decay W→lÎœW \to l\nu are obtained in the laboratory system. CP violation in the tt-production vertex is assumed. Different angular and total cross section CP violating asymmetries are considered. Relations testing CP violation solely in the tt-decay vertex are also obtained. A numerical analysis is performed in the MSSM with a CP violating phase of the trilinear coupling At~A_{\tilde t}. The asymmetries are typically of the order 10−310^{-3} - 10−410^{-4}.Comment: The numerical results are corrected and some changes that meet the requirements of Phys. Rev. D are mad

    H/A Higgs Mixing in CP-Noninvariant Supersymmetric Theories

    Full text link
    For large masses, the two heavy neutral Higgs bosons are nearly degenerate in many 2--Higgs doublet models, and particularly in supersymmetric models. In such a scenario the mixing between the states can be very large if the theory is CP-noninvariant. We analyze the formalism describing this configuration, and we point to some interesting experimental consequences.Comment: LaTeX, 1+20 pages, 6 figure

    CP violation in supersymmetric model with non-degenerate A-terms

    Get PDF
    We study the CP phases of the soft supersymmetry breaking terms in string-inspired models with non-universal trilinear couplings. We show that such non-universality plays an important role on all CP violating processes. In particular these new supersymmetric sources of CP violation may significantly contribute to the observed CP phenomena in kaon physics while respecting the severe bound on the electric dipole moment of the neutron.Comment: 14 pages, Late

    Ό→eÎł\mu \to e \gamma and Ό→3e\mu \to 3e processes with polarized muons and supersymmetric grand unified theories

    Full text link
    ÎŒ+→e+Îł\mu^{+} \to e^{+} \gamma and ÎŒ+→e+e+e−\mu^{+} \to e^{+}e^{+}e^{-} processes are analyzed in detail with polarized muons in supersymmetric grand unified theories. We first present Dalitz plot distribution for ÎŒ+→e+e+e−\mu^{+} \to e^{+}e^{+}e^{-} decay based on effective Lagrangian with general lepton-flavor-violating couplings and define various P- and T-odd asymmetries. We calculate branching ratios and asymmetries in supersymmetric SU(5) and SO(10) models taking into account complex soft supersymmetry breaking terms. Imposing constraints from experimental bounds on the electron, neutron and atomic electric dipole moments, we find that the T-odd asymmetry for ÎŒ+→e+e+e−\mu^{+} \to e^{+}e^{+}e^{-} can be 15% in the SU(5) case. P-odd asymmetry with respect to muon polarization for ÎŒ+→e+Îł\mu^{+} \to e^{+} \gamma varies from -20% to -100% for the SO(10) model while it is +100+100% in the SU(5) case. We also show that the P-odd asymmetries in ÎŒ+→e+e+e−\mu^{+} \to e^{+}e^{+}e^{-} and the ratio of ÎŒ+→e+e+e−\mu^{+} \to e^{+}e^{+}e^{-} and ÎŒ+→e+Îł\mu^{+} \to e^{+} \gamma branching fractions are useful to distinguish different models.Comment: 52 pages, 15 figure
    • 

    corecore