6,315 research outputs found

    T-odd generalized and quasi transverse momentum dependent parton distribution in a scalar spectator model

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    Generalized transverse momentum dependent parton distributions (GTMDs), as mother funtions of transverse momentum dependent parton distributions (TMDs) and generalized parton distributions (GPDs), encode the most general parton structure of hadrons. We calculate four twist-two time reversal odd GTMDs of pion in a scalar spectator model. We study the dependence of GTMDs on the longitudinal momentum fraction xx carried by the active quark and the transverse momentum ∣kβƒ—T∣|\vec k_T| for different values of skewness ΞΎ\xi defined as the longitudinal momentum transferred to the proton as well as the total momentum βˆ£Ξ”βƒ—T∣|\vec\Delta_T| transferred to the proton. In addition, the quasi-TMDs and quasi-GPDs of pion have also been investigated in this paper

    Searches for the Anomalous FCNC Top-Higgs Couplings with Polarized Electron Beam at the LHeC

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    In this paper, we study the single top and Higgs associated production eβˆ’pβ†’Ξ½etΛ‰β†’Ξ½ehqΛ‰(hβ†’bbΛ‰)\rm e^- p\rightarrow \nu_e \bar{t} \rightarrow \nu_e h \bar{q}(h\rightarrow b\bar{b}) in the top-Higgs FCNC couplings at the LHeC with the electron beam energy of EeE_{e} = 60 GeV and EeE_{e} = 120 GeV, combination of a 7 TeV and 50 TeV proton beam. With the possibility of e-beam polarization (pep_{e} = 0, Β±0.6\pm0.6), we distinct the Cut-based method and the Multivariate Analysis (MVA) based method, and compare with the current experimental and theoretical limits. It is shown that the branching ratio Br (tβ†’uh)\rm(t\to uh) can be probed to 0.113 (0.093) %\%, 0.071 (0.057) %\%, 0.030 (0.022) %\% and 0.024 (0.019) %\% with the Cut-based (MVA-based) analysis at (EpE_{p}, EeE_{e}) = (7 TeV, 60 GeV), (EpE_{p}, EeE_{e}) = (7 TeV, 120 GeV), (EpE_{p}, EeE_{e}) = (50 TeV, 60 GeV) and (EpE_{p}, EeE_{e}) = (50 TeV, 120 GeV) beam energy and 1Οƒ\sigma level. With the possibility of e-beam polarization, the expected limits can be probed down to 0.090 (0.073) %\%, 0.056 (0.045) %\%, 0.024 (0.018) %\% and 0.019 (0.015) %\%, respectively.Comment: 13pages, 5 figures. Advance in High Energy Physic

    Exploring the Anomalous Top-Higgs FCNC Couplings at the electron proton colliders

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    We perform an updated analysis on the searches for the anomalous FCNC Yukawa interactions between the top quark, the Higgs boson, and either an up or charm quark (tqh,Β q=u,Β c\rm tqh,\ q=u,\ c). We probe the observability of the FCNC top-Higgs couplings through the processes eβˆ’pβ†’Ξ½etΛ‰β†’Ξ½ehqΛ‰\rm e^- p\rightarrow \nu_e \bar{t} \rightarrow \nu_e h \bar{q} (signal.I) and Β eβˆ’pβ†’Ξ½ehb\rm \ e^- p \to \nu_e h b (singal.II) at the proposed electron proton (ep) colliders, where the Higgs boson decays to a bbΛ‰\rm b\bar{b} pair. We find that at the high luminosity (1 abβˆ’1\rm ab^{-1}) ep colliders where the electrons have a polarisation of 80%\rm 80\% and electron energy is typical 60 GeV, the 2Οƒ\sigma upper limit on Br(tβ†’uh)\rm Br(t\to uh) are 0.15Γ—10βˆ’20.15\times 10^{-2}(2.9Γ—10βˆ’42.9\times 10^{-4}) at the 7TeV@LHeC(50TeV@FCC-eh) for signal.I and 0.15Γ—10βˆ’20.15\times 10^{-2}(2.2Γ—10βˆ’42.2\times 10^{-4}) for signal.II. We also give an estimate on how the sensitivity (take signal.I as examples) would change when we reduce the electron beam energy from 60 GeV to 50 GeV or even 40 GeV due to the cost reason. The conclusion is that the discovery potential reduce 8.7%8.7\%(29.4%29.4\%) if the electron beam change from 60GeV to 50(40) GeV at the 7TeV LHeC, and 16.8%16.8\%(19.8%19.8\%) at the 50 TeV FCC-eh.Comment: 8 figures. 4 tables. 26 page

    A study of ion acceleration, asymmetric optical pumping and low frequency waves in two expanding helicon plasmas

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    This work concerns measurements of parallel ion flow, optical pumping, and low frequency waves in expanding plasmas generated by two different helicon plasma sources. The measurements confirm numerical predictions of the formation of a current-free double layer in a region of diverging magnetic field. With laser-induced fluorescence (LIF), the double layer structure in both helicon plasma sources was investigated through measurements of the bulk parallel ion flow speed. Both double layers have a total potential drop of 3-4 kTe and length scales smaller than ion-neutral mean-free-path. A stronger double layer, with a potential drop of ∼ 6kTe , was created in a uniform magnetic field region with a plasma limiting aperture plate. During the investigations of ion acceleration in expanding plasmas, a new phenomenon, asymmetrical optical pumping (AOP) due to the acceleration of ions in magnetic field gradient, was observed. The signature of AOP is a difference in the LIF emission amplitude from a pair of Zeeman-split ion states. A model that reproduces the dependence of the AOP on magnetic-field and ion-velocity gradients is described. With magnetic fluctuation probes, low frequency, transverse, electromagnetic waves were also identified in the expanding helicon plasma. The wave is localized to the vicinity of the maximum plasma density gradient and appears only at low neutral pressure. Based on the scaling of the wave frequency and amplitude with magnetic field strength, the wave was identified as the resistive drift Alfven wave
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