8,447 research outputs found

    Oscillating Asymmetric Sneutrino Dark Matter from the Maximally U(1)LU(1)_L Supersymmetric Inverse Seesaw

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    The inverse seesaw mechanism provides an attractive approach to generate small neutrino mass, which origins from a tiny U(1)LU(1)_L breaking. In this paper, we work in the supersymmetric version of this mechanism, where the singlet-like sneutrino could be an asymmetric dark matter (ADM) candidate in the maximally U(1)LU(1)_{L} symmetric limit. However, even a tiny Ξ΄m\delta m, the mass splitting between sneutrino and anti-sneutrino as a result of the tiny U(1)LU(1)_{L} breaking effect, could lead to fast oscillation between sneutrino and anti-sneutrino and thus spoils the ADM scenario. We study the evolution of this oscillation and find that a weak scale sneutrino, which tolerates a relatively larger Ξ΄m∼10βˆ’5\delta m\sim 10^{-5} eV, is strongly favored. We also investigate possible natural ways to realize that small Ξ΄m\delta m in the model.Comment: PLB versio

    A Typha Angustifolia-like MoS2/carbon nanofiber composite for high performance Li-S batteries

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    A Typha Angustifolia-like MoS2/carbon nanofiber composite as both a chemically trapping agent and redox conversion catalyst for lithium polysulfides has been successfully synthesized via a simple hydrothermal method. Cycling performance and coulombic efficiency have been improved significantly by applying the Typha Angustifolia-like MoS2/carbon nanofiber as the interlayer of a pure sulfur cathode, resulting in a capacity degradation of only 0.09% per cycle and a coulombic efficiency which can reach as high as 99%

    Inclusive weak-annihilation decays and lifetimes of beauty-charmed baryons

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    Imbalanced beauty-charmed baryons Ξbc+,0 \Xi_{bc}^{+,0} are of great significance to the development of heavy flavor physics. In this work, we study the inclusive weak-annihilation decays of Ξbc+,0\Xi_{bc}^{+,0} and their contributions to the Ξbc+,0\Xi_{bc}^{+,0} lifetimes. For the calculation of the inclusive Ξbc+,0β†’Xcs\Xi_{bc}^{+,0}\to X_{cs} decay width where XcsX_{cs} stands for the sum of the final states with charm number +1 and strange number -1, we work in the heavy diquark effective theory which provides us with a convenient technical tool to construct the operator product expansion. The Ξbc+,0\Xi_{bc}^{+,0} is considered to be a superposition of two states with one containing a spin-0 bcbc diquark and the other one containing a spin-1 bcbc diquark. It is found that both the Ξbc+,0\Xi_{bc}^{+,0} lifetimes and the Ξbc+,0β†’Xcs\Xi_{bc}^{+,0}\to X_{cs} branching ratios are very sensitive to the bcbc spin in Ξbc+,0\Xi_{bc}^{+,0}. As Ξbc+\Xi_{bc}^+ has a longer lifetime than Ξbc0\Xi_{bc}^{0} and bigger branching ratios of similar decay channels, the exclusive decays Ξbc+β†’D(βˆ—)+Ξ›\Xi_{bc}^+\to D^{(*)+}\Lambda, Ξbc+β†’Ξ›c+KΛ‰(βˆ—)0\Xi_{bc}^+\to \Lambda_c^+\bar{K}^{(*)0}, Ξbc+β†’D(βˆ—)+Kβˆ’p\Xi_{bc}^+\to D^{(*)+}K^-p, and Ξbc+β†’D0KΛ‰(βˆ—)0p\Xi_{bc}^+\to D^{0}\bar{K}^{(*)0}p are more promising for experimental searches of Ξbc+,0\Xi_{bc}^{+,0} at the LHC comparing with exclusive decay Ξbc0β†’D0pKβˆ’\Xi_{b c} ^{0} \to D^0pK^-.Comment: 7 pages, 4 figure

    Simulation Game For Room Design

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