15,356 research outputs found

    Next-to-leading-order QCD corrections to e+eβˆ’β†’H+Ξ³e^+e^-\to H+\gamma

    Full text link
    The associated production of Higgs boson with a hard photon at lepton collider, i.e., e+eβˆ’β†’HΞ³e^+e^-\to H\gamma, is known to bear a rather small cross section in Standard Model, and can serve as a sensitive probe for the potential new physics signals. Similar to the loop-induced Higgs decay channels Hβ†’Ξ³Ξ³,ZΞ³H\to \gamma\gamma, Z\gamma, the e+eβˆ’β†’HΞ³e^+e^-\to H\gamma process also starts at one-loop order provided that the tiny electron mass is neglected. In this work, we calculate the next-to-leading-order (NLO) QCD corrections to this associated H+Ξ³H+\gamma production process, which mainly stem from the gluonic dressing to the top quark loop. The QCD corrections are found to be rather modest at lower center-of-mass energy range (s<300\sqrt{s}<300 GeV), thus of negligible impact on Higgs factory such as CEPC. Nevertheless, when the energy is boosted to the ILC energy range (sβ‰ˆ400\sqrt{s}\approx 400 GeV), QCD corrections may enhance the leading-order cross section by 20%20\%. In any event, the e+eβˆ’β†’HΞ³e^+e^-\to H\gamma process has a maximal production rate Οƒmaxβ‰ˆ0.08\sigma_{\rm max}\approx 0.08 fb around s=250\sqrt{s}= 250 GeV, thus CEPC turns out to be the best place to look for this rare Higgs production process. In the high energy limit, the effect of NLO QCD corrections become completely negligible, which can be simply attributed to the different asymptotic scaling behaviors of the LO and NLO cross sections, where the former exhibits a milder decrement ∝1/s\propto 1/s , but the latter undergoes a much faster decrease ∝1/s2\propto 1/s^2.Comment: v4, 11 pages, 6 figures, 2 tables; errors in Appendix are fixed; version accepted for publication at PL

    Holographic R\'enyi entropy in AdS3_3/LCFT2_2 correspondence

    Get PDF
    The recent study in AdS3_3/CFT2_2 correspondence shows that the tree level contribution and 1-loop correction of holographic R\'enyi entanglement entropy (HRE) exactly match the direct CFT computation in the large central charge limit. This allows the R\'enyi entanglement entropy to be a new window to study the AdS/CFT correspondence. In this paper we generalize the study of R\'enyi entanglement entropy in pure AdS3_3 gravity to the massive gravity theories at the critical points. For the cosmological topological massive gravity (CTMG), the dual conformal field theory (CFT) could be a chiral conformal field theory or a logarithmic conformal field theory (LCFT), depending on the asymptotic boundary conditions imposed. In both cases, by studying the short interval expansion of the R\'enyi entanglement entropy of two disjoint intervals with small cross ratio xx, we find that the classical and 1-loop HRE are in exact match with the CFT results, up to order x6x^6. To this order, the difference between the massless graviton and logarithmic mode can be seen clearly. Moreover, for the cosmological new massive gravity (CNMG) at critical point, which could be dual to a logarithmic CFT as well, we find the similar agreement in the CNMG/LCFT correspondence. Furthermore we read the 2-loop correction of graviton and logarithmic mode to HRE from CFT computation. It has distinct feature from the one in pure AdS3_3 gravity.Comment: 28 pages. Typos corrected, published versio

    Interaction effect in two-dimensional Dirac fermions

    Get PDF
    Based on the Dirac equations in the two-dimensional Ο€βˆ’\pi- flux model, we study the interaction effects both in nontrivial gapped and gapless Dirac equations with numerical exact diagonalization method. In the presence of the nearest and next nearest neighbor interactions: for nontrivial gapped Dirac equation, the topological phase is robust and persists in a finite region of the phase diagram; while for gapless Dirac equation, charge-density-wave and stripe phases are identified and the phase diagram in (V1,V2)(V_1, V_2) plane is obtained. When the next-next-nearest neighbor interaction is further included to gapless Dirac equation, the topological phase expected in the mean-field theory is absent. Our results are related to the possibility of dynamically generating topological phase from the electronic correlations.Comment: 7 pages, 8 figures. More discussins are added; accepted for publication in Physical Review
    • …
    corecore