393 research outputs found

    Decaying neutralino dark matter in anomalous U(1)HU(1)_H models

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    In supersymmetric models extended with an anomalous U(1)HU(1)_H different R-parity violating couplings can yield an unstable neutralino. We show that in this context astrophysical and cosmological constraints on neutralino decaying dark matter forbid bilinear R-parity breaking neutralino decays and lead to a class of purely trilinear R-parity violating scenarios in which the neutralino is stable on cosmological scales. We have found that among the resulting models some of them become suitable to explain the observed anomalies in cosmic-ray electron/positron fluxes.Comment: 19 pages, 3 figures. References added, typos corrected, accepted version in Phys Rev

    Bounds on Broken R-Parity from Leptonic Meson Decays

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    Investigating leptonic decays of pi^-, K^-, B^-, pi^0, K_L^0, B_s^0 we present new bounds on some products of two R-parity violating coupling constants. For mesons of a similar structure but so far poor experimental data we give the corresponding formulae, to be used in the future.Comment: Latex, 15 pages, 1 figure; final version which appeared in Phys.Rev.

    Minimal supersymmetric standard model with gauge mediated supersymmetry breaking and neutrinoless double beta decay

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    The Minimal Supersymmetric Standard Model with gauge mediated supersymmetry breaking and trilinear R-parity violation is applied to the description of neutrinoless double beta decay. A detailed study of limits on the parameter space coming from the B to (X,gamma) processes by using the recent CLEO results is performed. The importance of two-nucleon and pion-exchange realizations of neutrinoless double beta decay together with gluino and neutralino contributions to this process are addressed. We have deduced new limits on the trilinear R-parity breaking parameter lambda_{111}' from the non-observability of 0 nu beta beta in several medium and heavy open-shell nuclei for different gauge mediated breaking scenarios. In general, they are stronger than those known from other analyses. Also some studies with respect to the future neutrinoless double beta decay projects are presented.Comment: 10 pages, 7 figure

    Neutrino masses in SU(5)×U(1)FSU(5)\times U(1)_F with adjoint flavons

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    We present a SU(5)×U(1)FSU(5)\times U(1)_F supersymmetric model for neutrino masses and mixings that implements the seesaw mechanism by means of the heavy SU(2) singlets and triplets states contained in three adjoints of SU(5). We discuss how Abelian U(1)FU(1)_F symmetries can naturally yield non-hierarchical light neutrinos even when the heavy states are strongly hierarchical, and how it can also ensure that RR--parity arises as an exact accidental symmetry. By assigning two flavons that break U(1)FU(1)_F to the adjoint representation of SU(5) and assuming universality for all the fundamental couplings, the coefficients of the effective Yukawa and Majorana mass operators become calculable in terms of group theoretical quantities. There is a single free parameter in the model, however, at leading order the structure of the light neutrinos mass matrix is determined in a parameter independent way.Comment: 16 pages, 9 figures. Included contributions to neutrino masses from the triplet states contained in the three adjoints of SU(5

    Like Sign Dilepton Signature for R-Parity Violating SUSY Search at the Tevatron Collider

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    The like sign dileptons provide the most promising signature for superparticle search in a large category of RR-parity violating SUSY models. We estimate the like sign dilepton signals at the Tevatron collider, predicted by these models, over a wide region of the MSSM parameter space. One expects an unambiguous signal upto a gluino mass of 200300200 - 300 GeV (500\geq 500 GeV) with the present (proposed) accumulated luminosity of 0.1 (1) fb1\sim 0.1~(1)~{\rm fb}^{-1}.Comment: 12 page LaTeX file; 5 figures available upon request from the autho

    CP asymmetries in the supersymmetric trilepton signal at the LHC

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    In the CP-violating Minimal Supersymmetric Standard Model, we study the production of a neutralino-chargino pair at the LHC. For their decays into three leptons, we analyze CP asymmetries which are sensitive to the CP phases of the neutralino and chargino sector. We present analytical formulas for the entire production and decay process, and identify the CP-violating contributions in the spin correlation terms. This allows us to define the optimal CP asymmetries. We present a detailed numerical analysis of the cross sections, branching ratios, and the CP observables. For light neutralinos, charginos, and squarks, the asymmetries can reach several 10%. We estimate the discovery potential for the LHC to observe CP violation in the trilepton channel.Comment: 39 pages, 8 figures, version to appear in EPJC, discussion(s) added, typo in (D.79), (D.118) corrected, new Fig. 7; The European Physical Journal C, Volume 72, Issue 3, 201

    Like Sign Dilepton Signature for Gluino Production at LHC with or without R Conservation

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    The isolated like sign dilepton signature for gluino production is investigated at the LHC energy for the RR conserving as well as the LL and BB violating SUSY models over a wide range of the parameter space. One gets viable signals for gluino masses of 300 and 600 GeV for both RR conserving and LL violating models, while it is less promising for the BB violating case. For a 1000 GeV gluino, the LL violating signal should still be viable; but the RR conserving signal becomes too small at least for the low luminosity option of LHC.Comment: (e-mail: [email protected]) Latex: No. of pages 21, no. of figures 6 - available on reques

    Impact of R-Parity Violation on Supersymmetry Searches at the Tevatron

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    We evaluate cross sections for \eslt, 1\ell and various dilepton and multilepton event topologies that result from the simultaneous production of all sparticles at the Tevatron collider, both within the minimal model framework as well as in two different RR-parity violating scenarios. Our analysis assumes that these RR-violating couplings are small, and that their sole effect is to cause the lightest supersymmetric particle to decay inside the detector. We reassess future strategies for sparticle searches at the Tevatron, and quantify by how much the various signals for supersymmetry could differ from their minimal model expectations, if RR-parity is not conserved due to either baryon number or lepton number violating operators. We also evaluate the Tevatron reach in mtgm_{\tg} for the various models, and find that rate-limited multilepton signals ultimately provide the largest reach for both RR-parity conserving and RR-parity violating cases.Comment: preprint nos. FSU-HEP-941001, UR-1387, ER-40685-836 and UH-511-807-94, 13 pages (REVTEX) plus 3 uuencoded figures attache

    A remark on sphaleron erasure of baryon asymmetry

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    We complete an existing result for how the baryon asymmetry left over after a period of full thermal equilibrium depends on different lepton asymmetries.Comment: 5 pages; small clarifications and a reference added; to appear in PR

    The Supersymmetric Standard Models with Decay and Stable Dark Matters

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    We propose two supersymmetric Standard Models (SMs) with decaying and stable dark matter (DM) particles. To explain the SM fermion masses and mixings and have a heavy decay DM particle S, we consider the Froggatt-Nielsen mechanism by introducing an anomalous U(1)_X gauge symmetry. Around the string scale, the U(1)_X gauge symmetry is broken down to a Z_2 symmetry under which S is odd while all the SM particles are even. S obtains a vacuum expectation value around the TeV scale, and then it can three-body decay dominantly to the second/third family of the SM leptons in Model I and to the first family of the SM leptons in Model II. Choosing a benchmark point in the constrained minimal supersymmetric SM with exact R parity, we show that the lightest neutralino DM is consistent with the CDMS II experiment. Considering S three-body decay and choosing suitable parameters, we show that the PAMELA and Fermi-LAT experiments and the PAMELA and ATIC experiments can be explained in Model I and Model II, respectively.Comment: RevTex4, 26 pages, 6 figures, references added, version to appear in EPJ
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