3,248 research outputs found

    Enhancing li→3ljl_i \to 3 l_j with the Z0Z^0-penguin

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    Lepton flavor violation (LFV) has been observed in neutrino oscillations. For charged lepton FV decays only upper limits are known, but sizable branching ratios are expected in many neutrino mass models. High scale models, such as the classical supersymmetric seesaw, usually predict that decays li→3ljl_i \to 3 l_j are roughly a factor α\alpha maller than the corresponding decays li→ljγl_i \to l_j \gamma. Here we demonstrate that the Z0Z^0-penguin diagram can give an enhancement for decays li→3ljl_i \to 3 l_j in many extensions of the MSSM. We first discuss why the Z0Z^0-penguin is not dominant in the MSSM with seesaw and show that much larger contributions from the Z0Z^0-penguin are expected in general. We then demonstrate the effect numerically in two example models, namely, the supersymmetric inverse seesaw and R-parity violating supersymmetry.Comment: 5 pages; v2: minor corrections, final version to appear in PR

    Cooperation of Accountants with Bench and Bar

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    Income tax guide: an analysis of the obligations imposed on individuals, firms and corporations by the federal income tax law, suggestions for making returns, and form for recording income

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    The obligations imposed by the far reaching income tax law which has just been enacted may be broadly separated between those imposed on Individuals and those imposed on Corporations

    Fallacies of the Sales Tax

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    How to Write a Report

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    Certified public accountant

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    What the Certified Public Accountant is and what he does. The growth, the requirements and the work of a new profession. Reprinted from The business World, of JULY, 1910. With the Compliments of Lybrand, Ross Bros. & Montgomery Certified Public Accountants New York Pittsburgh Chicago Philadelphi

    Lepton flavor violation in low-scale seesaw models: SUSY and non-SUSY contributions

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    Taking the supersymmetric inverse seesaw mechanism as the explanation for neutrino oscillation data, we investigate charged lepton flavor violation in radiative and 3-body lepton decays as well as in neutrinoless μ−e\mu-e conversion in muonic atoms. In contrast to former studies, we take into account all possible contributions: supersymmetric as well as non-supersymmetric. We take CMSSM-like boundary conditions for the soft supersymmetry breaking parameters. We find several regions where cancellations between various contributions exist, reducing the lepton flavor violating rates by an order of magnitude compared to the case where only the dominant contribution is taken into account. This is in particular important for the correct interpretation of existing data as well as for estimating the reach of near future experiments where the sensitivity will be improved by one to two orders of magnitude. Moreover, we demonstrate that ratios like BR(τ→3μ\tau\to 3 \mu)/BR(τ→μe+e−\tau\to \mu e^+ e^-) can be used to determine whether the supersymmetric contributions dominate over the W±W^\pm and H±H^\pm contributions or vice versa.Comment: 75 pages, 7 figures. v3: references and comments added. Matches published versio

    Phenomenology of the minimal supersymmetric U(1)B−L×U(1)RU(1)_{B-L}\times U(1)_R extension of the standard model

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    We discuss the minimal supersymmetric U(1)B−L×U(1)RU(1)_{B-L}\times U(1)_R extension of the standard model. Gauge couplings unify as in the MSSM, even if the scale of U(1)B−L×U(1)RU(1)_{B-L}\times U(1)_R breaking is as low as order TeV and the model can be embedded into an SO(10) grand unified theory. The phenomenology of the model differs in some important aspects from the MSSM, leading potentially to rich phenomenology at the LHC. It predicts more light Higgs states and the mostly left CP-even Higgs has a mass reaching easily 125 GeV, with no constraints on the SUSY spectrum. Right sneutrinos can be the lightest supersymmetric particle, changing all dark matter constraints on SUSY parameter space. The model has seven neutralinos and squark/gluino decay chains involve more complicated cascades than in the MSSM. We also discuss briefly low-energy and accelerator constraints on the model, where the most important limits come from recent Z′Z' searches at the LHC and upper limits on lepton flavour violation.Comment: 46 pages, 11 figure
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