42,801 research outputs found

    Enhancing thjthj Production from Top-Higgs FCNC Couplings

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    In this paper, we study the single top and Higgs associated production ppβ†’thjpp \to thj in the presence of top-Higgs FCNC couplings(ΞΊtqh,q=u,c\kappa_{tqh}, q=u,c) at the LHC. Under the current constraints, we find that the cross section of ppβ†’thjpp \to thj can be sizably enhanced in comparison with the SM predictions at 8 and 14 TeV LHC. We also find that the full cross section of ppβ†’thjpp \to thj with ΞΊtch\kappa_{tch} is larger than the resonant cross section of ppβ†’ttΛ‰β†’thjpp \to t\bar{t} \to thj by a factor 1.16 at 8 TeV LHC and 1.12 at 14 TeV LHC, respectively. We further explore the observability of top-Higgs FCNC couplings through ppβ†’t(β†’bβ„“+Ξ½β„“)h(β†’Ξ³Ξ³)jpp \to t(\to b\ell^{+} \nu_{\ell}) h( \to \gamma\gamma) j and find that the branching ratios Br(tβ†’qh)Br(t\to qh), Br(tβ†’uh)Br(t \to uh) and Br(tβ†’ch)Br(t \to ch) can be respectively probed to 0.12%,Β 0.23%0.12\%,~0.23\% and Β 0.26%~0.26\% at 3Οƒ3\sigma sensitivity at 14 TeV LHC with L=3000{\cal L} =3000 fbβˆ’1^{-1}.Comment: 15 pages, 7 figures, references and discussions added, accepted by JHE

    Onsager Relations and Hydrodynamic Balance Equations in 2D Quantum Wells

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    In this letter we clarify the role of heat flux in the hydrodynamic balance equations in 2D quantum wells, facilitating the formulation of an Onsager relation within the framework of this theory. We find that the Onsager relation is satisfied within the framework of the 2D hydrodynamic balance equation transport theory at sufficiently high density. The condition of high density is consonant with the requirement of strong electron-electron interactions for the validity of our balance equation formulation.Comment: 11 pages, RevTex, 4 postscript figures are avaliable upon reques

    Numerical investigation of the radial quadrupole and scissors modes in trapped gases

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    The analytical expressions for the frequency and damping of the radial quadrupole and scissors modes, as obtained from the method of moments, are limited to the harmonic potential. In addition, the analytical results may not be suciently accurate as an average relaxation time is used and the high-order moments are ignored. Here, we propose to numerically solve the Boltzmann model equation in the hydrodynamic, transition, and collisionless regimes to study mode frequency and damping. When the gas is trapped by the harmonic potential, we nd that the analytical expressions underestimate the damping in the transition regime. In addition, we demonstrate that the numerical simulations are able to provide reasonable predictions for the collective oscillations in the Gaussian potentials
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