34,939 research outputs found

    Quantum Phase Transition in Hall Conductivity on an Anisotropic Kagome Lattice

    Full text link
    We study the quantum Hall effect(QHE) on the Kagom\'{e} lattice with anisotropy in one of the hopping integrals. We find a new type of QHE characterized by the quantization rules for Hall conductivity σxy=2ne2/h\sigma_{xy}=2ne^{2}/h and Landau Levels E(n)=±vF(n+1/2)BeE(n)=\pm v_{F}\sqrt{(n+1/2)\hbar Be} (nn is an integer), which is different from any known type. This phase evolves from the QHE phase with σxy=4(n+1/2)e2/h\sigma_{xy}=4(n+1/2)e^{2}/h and E(n)=±vF2nBeE(n)=\pm v_{F}\sqrt{2n\hbar Be} in the isotropic case, which is realized in a system with massless Dirac fermions (such as in graphene). The phase transition does not occur simultaneously in all Hall plateaus as usual but in sequence from low to high energies, with the increase of hopping anisotropy.Comment: 5 pages, 4 figure

    SU(5) Symmetry of spdfg Interacting Boson Model

    Get PDF
    The extended interacting boson model with s-, p-, d-, f- and g-bosons being included (spdfg IBM) are investigated. The algebraic structure including the generators, the Casimir operators of the groups at the SU(5) dynamical symmetry and the branching rules of the irreducible representation reductions along the group chain are obtained. The typical energy spectrum of the Symmetry is given.Comment: 12 pages, 2 figure

    CPCP violation in charmed hadron decays into neutral kaons

    Full text link
    We find a new CPCP violating effect in charmed hadron decays into neutral kaons, which is induced by the interference between the Cabibbo-favored and doubly Cabibbo-suppressed amplitudes with the K0K0K^{0}-\overline K^{0} mixing. It is estimated to be of order of O(103)\mathcal{O}(10^{-3}), much larger than the direct CPCP asymmetry, but missed in the literature. To reveal this new CPCP violation effect, we propose a new observable, the difference of the CPCP asymmetries in the D+π+KS0D^{+}\to \pi^{+}K_S^0 and Ds+K+KS0D_{s}^{+}\to K^{+} K_S^0 modes. Once the new effect is determined by experiments, the direct CPCP asymmetry then can be extracted and used to search for new physics.Comment: 6 pages, 3 figures. Contribution to the proceeding of The 15th International Conference on Flavor Physics & CP Violation, 5-9 June 2017, Prague, Czech Republi

    Soft gluon resummation in the signal-background interference process of gg(h)ZZgg(\to h^*) \to ZZ

    Get PDF
    We present a precise theoretical prediction for the signal-background interference process of gg(h)ZZgg(\to h^*) \to ZZ, which is useful to constrain the Higgs boson decay width and to measure Higgs couplings to the SM particles. The approximate NNLO KK-factor is in the range of 2.052.452.05-2.45 (1.852.251.85-2.25), depending on MZZM_{ZZ}, at the 8 (13) TeV LHC. And the soft gluon resummation can increase the approximate NNLO result by about 10%10\% at both the 8 TeV and 13 TeV LHC. The theoretical uncertainties including the scale, uncalculated multi-loop amplitudes of the background and PDF+αs+\alpha_s are roughly O(10%)\mathcal{O}(10\%) at NNLL{\rm NNLL'}. We also confirm that the approximate KK-factors in the interference and the pure signal processes are the same.Comment: 18 pages, 9 figures; v2 published in JHE

    A 1+5-dimensional gravitational-wave solution: curvature singularity and spacetime singularity

    Full text link
    We solve a 1+51+5-dimensional cylindrical gravitational-wave solution of the Einstein equation, in which there are two curvature singularities. Then we show that one of the curvature singularities can be removed by an extension of the spacetime. The result exemplifies that the curvature singularity is not always a spacetime singularity; in other words, the curvature singularity cannot serve as a criterion for spacetime singularities

    Why the entropy of spacetime is independent of species of particles -- the species problem

    Full text link
    The Hawking radiation emits all species of particles, but the Bekenstein-Hawking entropy is independent of the number of the species of particles. This is the so-called species problem --- a puzzling problem for a long time. In this paper, we suggest a solution to this problem. A result of the scheme is that the black hole atmosphere has a mass equaling 3/8 mass of a classical Schwarzschild black hole, which agrees with 't Hooft's brick wall model

    Implications on the first observation of charm CPV at LHCb

    Full text link
    Very recently, the LHCb Collaboration observed the CPCP violation (CPV) in the charm sector for the first time, with ΔACPdirACP(D0K+K)ACP(D0π+π)=(1.54±0.29)×103\Delta A_{CP}^{\rm dir}\equiv A_{CP}(D^0\to K^+K^-)-A_{CP}(D^0\to \pi^+\pi^-)=(-1.54\pm0.29)\times10^{-3}. This result is consistent with our prediction of ΔACPSM=(0.571.87)×103\Delta A_{CP}^{\rm SM}=(-0.57\sim -1.87)\times 10^{-3} obtained in the factorization-assisted topological-amplitude (FAT) approach in [PRD86,036012(2012)]. It implies that the current understanding of the penguin dynamics in charm decays in the Standard Model is reasonable. Motivated by the success of the FAT approach, we further suggest to measure the D+K+Kπ+D^+\to K^+K^-\pi^+ decay, which is the next potential mode to reveal the CPV of the same order as 10310^{-3}.Comment: 10 page
    corecore