3,751 research outputs found

    The semileptonic baryonic decay Ds+→ppˉe+νeD_s^+\to p\bar p e^+ \nu_e

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    The decay Ds+β†’ppΛ‰e+Ξ½eD_s^+\to p \bar p e^+\nu_e with a proton-antiproton pair in the final state is unique in the sense that it is the only semileptonic baryonic decay which is physically allowed in the charmed meson sector. Its measurement will test our basic knowledge on semileptonic Ds+D_s^+ decays and the low-energy ppΛ‰p\bar p interactions. Taking into account the major intermediate state contributions from Ξ·,Ξ·β€²,f0(980)\eta, \eta', f_0(980) and X(1835)X(1835), we find that its branching fraction is at the level of 10βˆ’9∼10βˆ’810^{-9} \sim 10^{-8}. The location and the nature of X(1835)X(1835) state are crucial for the precise determination of the branching fraction. We wish to trigger a new round of a careful study with the upcoming more data in BESIII as well as the future super tau-charm factory.Comment: final version, accepted for publication in Phys. Lett.

    Branching fractions of semileptonic DD and DsD_s decays from the covariant light-front quark model

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    Based on the predictions of the relevant form factors from the covariant light-front quark model, we show the branching fractions for the D(Ds)β†’(P, S, V, A) ℓνℓD (D_s) \to (P,\,S,\,V,\,A)\,\ell\nu_\ell (β„“=e\ell=e or ΞΌ\mu) decays, where PP denotes the pseudoscalar meson, SS the scalar meson with a mass above 1 GeV, VV the vector meson and AA the axial-vector one. Comparison with the available experimental results are made, and we find an excellent agreement. The predictions for other decay modes can be tested in a charm factory, e.g., the BESIII detector. The future measurements will definitely further enrich our knowledge on the hadronic transition form factor as well as the inner structure of the even-parity mesons (SS and AA).Comment: Predictions on D-> K1(1270), K1(1400) l nu rates correcte

    Thermoelectric DC conductivities with momentum dissipation from higher derivative gravity

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    We present a mechanism of momentum relaxation in higher derivative gravity by adding linear scalar fields to the Gauss-Bonnet theory. We analytically computed all of the DC thermoelectric conductivities in this theory by adopting the method given by Donos and Gauntlett in [arXiv:1406.4742]. The results show that the DC electric conductivity is not a monotonic function of the effective impurity parameter Ξ²\beta: in the small Ξ²\beta limit, the DC conductivity is dominated by the coherent phase, while for larger Ξ²\beta, pair creation contribution to the conductivity becomes dominant, signaling an incoherent phase. In addition, the DC heat conductivity is found independent of the Gauss-Bonnet coupling constant.Comment: 1+19 pages, 2 figures,typos in Eq.(40) correcte

    Anisotropic plasma with a chemical potential and scheme-independent instabilities

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    Generically, the black brane solution with planar horizons is thermodynamically stable. We find a counter-example to this statement by demonstrating that an anisotropic black brane is unstable. We present a charged black brane solution dual to a spatially anisotropic finite temperature N=4\mathcal{N}=4 super Yang-Mills plasma at finite U(1)U(1) chemical potential. This static and regular solution is obtained both numerically and analytically. We uncover rich thermodynamic phase structures for this system by considering the cases when the anisotropy constant "a" takes real and imaginary values, respectively. In the case a2>0a^2>0, the phase structure of this anisotropic black brane is similar to that of Schwarzschild-AdS black hole with S3S^3 horizon topology, yielding a thermodynamical instability at smaller horizon radii. For the condition a2≀0a^2\leq 0, the thermodynamics is dominated by the black brane phase for all temperatures.Comment: 14pages,14figures, minor changes, PLB in pres

    Random Sampling of Bandlimited Graph Signals from Local Measurements

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    The random sampling on graph signals is one of the fundamental topics in graph signal processing. In this letter, we consider the random sampling of k-bandlimited signals from the local measurements and show that no more than O(klogk) measurements with replacement are sufficient for the accurate and stable recovery of any k-bandlimited graph signals. We propose two random sampling strategies based on the minimum measurements, i.e., the optimal sampling and the estimated sampling. The geodesic distance between vertices is introduced to design the sampling probability distribution. Numerical experiments are included to show the effectiveness of the proposed methods
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