7,842 research outputs found

    Unifying gauge couplings at the string scale

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    Using the current precision electroweak data, we look for the minimal particle content which is necessary to add to the standard model in order to have a complete unification of gauge couplings and gravity at the weakly coupled heterotic string scale. We find that the addition of a vector-like fermion at an intermediate scale and a non-standard hypercharge normalization are in general sufficient to achieve this goal at two-loop level. Requiring the extra matter scale to be below the TeV scale, it is found that the addition of three vector-like fermion doublets with a mass around 700 GeV yields a perfect string-scale unification, provided that the affine levels are (kY,k2,k3)=(13/3,1,2)(k_Y, k_2 ,k_3)=(13/3, 1, 2) , as in the SU(5)×SU(5)SU(5) \times SU(5) string-GUT. Furthermore, if supersymmetry is broken at the unification scale, the Higgs mass is predicted in the range 125 GeV - 170 GeV, depending on the precise values of the top quark mass and tanβ\tan \beta parameter.Comment: 11 pages, 4 eps figures, using jpconf style, talk given at CORFU2005, RTN meeting ``The Quest for Unification: Theory Confronts Experiment'', 11 - 18 September 2005, Corfu, Greec

    Physics Behind Precision

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    This document provides a writeup of contributions to the FCC-ee mini-workshop on "Physics behind precision" held at CERN, on 2-3 February 2016.Comment: https://indico.cern.ch/event/469561

    Simulating the High Energy Gamma-ray sky seen by the GLAST Large Area Telescope

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    This paper presents the simulation of the GLAST high energy gamma-ray telescope. The simulation package, written in C++, is based on the Geant4 toolkit, and it is integrated into a general framework used to process events. A detailed simulation of the electronic signals inside Silicon detectors has been provided and it is used for the particle tracking, which is handled by a dedicated software. A unique repository for the geometrical description of the detector has been realized using the XML language and a C++ library to access this information has been designed and implemented. A new event display based on the HepRep protocol was implemented. The full simulation was used to simulate a full week of GLAST high energy gamma-ray observations. This paper outlines the contribution developed by the Italian GLAST software group.Comment: 6 pages, 4 figures, to be published in the Proceedings of the 6th International Symposium ''Frontiers of Fundamental and Computational Physics'' (FFP6), Udine (Italy), Sep. 26-29, 200

    The littlest Higgs model and Higgs boson associated production with top quark pair at high energy linear e+ee^{+}e^{-} collider

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    In the parameter space allowed by the electroweak precision measurement data, we consider the contributions of the new particles predicted by the littlest Higgs(LHLH) model to the Higgs boson associated production with top quark pair in the future high energy linear e+ee^{+}e^{-} collider(ILCILC). We find that the contributions mainly come from the new gauge bosons ZHZ_{H} and BHB_{H}. For reasonable values of the free parameters, the absolute value of the relative correction parameter δσ/σSM\delta\sigma/\sigma^{SM} can be significanly large, which might be observed in the future ILCILC experiment with S=800GeV\sqrt{S}=800GeV.Comment: latex files, 13 pages, 3 figure

    Flavor changing scalar couplings and tγ(Z)t\gamma(Z) production at hadron colliders

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    We calculate the contributions of the flavor changing scalar (FCSFCS) couplings arised from topcolor-assisted technicolor (TC2TC2) models at tree-level to the tγt\gamma and tZtZ production at the Tevatron and LHCLHC experiments. We find that the production cross sections are very small at the Tevatron with s=1.96TeV\sqrt{s}=1.96TeV, which is smaller than 5 fb in most of the parameter space of TC2TC2 models. However, the virtual effects of the FCSFCS couplings on the tγ(Z)t\gamma(Z) production can be easily detected at the LHCLHC with s=14TeV\sqrt{s}=14TeV via the final state γlνˉb\gamma l\bar{\nu}b (l+llνˉbl^{+}l^{-}l\bar{\nu}b).Comment: 10 pages,5 figure
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