20,798 research outputs found

    Gauge glass in two dimensions

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    The gauge glass model offers an interesting example of a randomly frustrated system with a continuous O(2) symmetry. In two dimensions, the existence of a glass phase at low temperatures has long been disputed among numerical studies. To resolve this controversy, we examine the behavior of vortices whose movement generates phase slips that destroy phase rigidity at large distances. Detailed analytical and numerical studies of the corresponding Coulomb gas problem in a random potential establish that the ground state, with a finite density of vortices, is polarizable with a scale-dependent dielectric susceptibility. Screening by vortex/antivortex pairs of arbitrarily large size is present to eliminate the logarithmic divergence of the Coulomb energy of a single vortex. The observed power-law decay of the Coulomb interaction between vortices with distance in the ground state leads to a power-law divergence of the glass correlation length with temperature TT. It is argued that free vortices possess a bound excitation energy and a nonzero diffusion constant at any T>0T>0.Comment: 10 pages, no figure, to appear in Proceedings of YKIS 2009 Workshop: Frontiers of Nonequilibrium Physic

    Study of the heavy CP-even Higgs with mass 125 GeV in two-Higgs-doublet models at the LHC and ILC

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    We assume that the 125 GeV Higgs discovered at the LHC is the heavy CP-even Higgs of the two-Higgs-doublet models, and examine the parameter space in the Type-I, Type-II, Lepton-specific and Flipped models allowed by the latest Higgs signal data, the relevant experimental and theoretical constraints. Further, we show the projected limits on tanβ\tan\beta, sin(βα)\sin(\beta-\alpha), HffˉHf\bar{f} and HVVHVV couplings from the future measurements of the 125 GeV Higgs at the LHC and ILC, including the LHC with integrated luminosity of 300 fb1^{-1} (LHC-300 fb1^{-1}) and 3000 fb1^{-1} (LHC-3000 fb1^{-1}) as well as the ILC at s=250\sqrt{s}=250 GeV (ILC-250 GeV), s=500\sqrt{s}=500 GeV (ILC-500 GeV) and s=1000\sqrt{s}=1000 GeV (ILC-1000 GeV). Assuming that the future Higgs signal data have no deviation from the SM expectation, the LHC-300 fb1^{-1}, LHC-3000 fb1^{-1} and ILC-1000 GeV can exclude the wrong-sign Yukawa coupling regions of the Type-II, Flipped and Lepton-specific models at the 2σ2\sigma level, respectively. The future experiments at the LHC and ILC will constrain the Higgs couplings to be very close to SM values, especially for the HVVHVV coupling.Comment: 22 pages, 3 tables, 6 figures. Version accepted for publication in JHE

    Rare-event induced binding transition of heteropolymers

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    Sequence heterogeneity broadens the binding transition of a polymer onto a linear or planar substrate. This effect is analyzed in a real-space renormalization group scheme designed to capture the statistics of rare events. In the strongly disordered regime, binding initiates at an exponentially rare set of ``good contacts''. Renormalization of the contact potential yields a Kosterlitz-Thouless type transition in any dimension. This and other predictions are confirmed by extensive numerical simulations of a directed polymer interacting with a columnar defect.Comment: 4 pages, 3 figure

    A simplified 2HDM with a scalar dark matter and the galactic center gamma-ray excess

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    Due to the strong constrain from the LUX experiment, the scalar portal dark matter can not generally explain a gamma-ray excess in the galactic center by the annihilation of dark matter into bbˉb\bar{b}. With the motivation of eliminating the tension, we add a scalar dark matter to the aligned two-Higgs-doublet model, and focus on a simplified scenario, which has two main characteristics: (i) The heavy CP-even Higgs is the discovered 125 GeV Higgs boson, which has the same couplings to the gauge bosons and fermions as the SM Higgs. (ii) Only the light CP-even Higgs mediates the dark matter interactions with SM particles, which has no couplings to WWWW and ZZZZ, but the independent couplings to the up-type quarks, down-type quarks and charged leptons. We find that the tension between SSbbˉ_{SS\to b\bar{b}} and the constraint from LUX induced by the scalar portal dark matter can go away for the isospin-violating dark matter-nucleon coupling with 1.0<fn/fp<0.7-1.0< f^n/f^p<0.7, and the constraints from the Higgs search experiments and the relic density of Planck are also satisfied.Comment: 12 pages, 3 figures, 1 table; reference adde

    Status of the aligned two-Higgs-doublet model confronted with the Higgs data

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    Imposing the theoretical constraints from vacuum stability, unitarity and perturbativity as well as the experimental constraints from the electroweak precision data, flavor observables and the non-observation of additional Higgs at collider, we study the implications of available Higgs signals on a two-Higgs-doublet model with the alignment of the down-type quarks and charged lepton Yukawa coupling matrices. Compared to the four traditional types of two-Higgs-doublet models, the model has two additional mixing angles θd\theta_d and θl\theta_l in the down-type quark and charged lepton Yukawa interactions. We find that the mixing angle θd\theta_d can loose the constraints on sin(βα)sin(\beta-\alpha), tanβtan\beta and mH±m_{H^{\pm}} sizably. The model can provide the marginally better fit to available Higgs signals data than SM, which requires the Higgs couplings with gauge bosons, uuˉu\bar{u} and ddˉd\bar{d} to be properly suppressed, and favors (1 <\theta_d< 2, 0.5 <\theta_l< 2.2) for mh=m_h= 125.5 GeV and (0.5 <\theta_d< 2, 0.5 <\theta_l< 2.2) for mH=m_H= 125.5 GeV. However, these Higgs couplings are allowed to have sizable deviations from SM for (mh=m_h= 125.5 GeV, 125.5 mH\leq m_H\leq 128 GeV) and (125 GeV mh\leq m_h\leq 125.5 GeV, mH=m_H= 125.5 GeV).Comment: 21 pages, 9 figures and 3 tables. Final version appeared in JHE
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