12,060 research outputs found

    Non-magnetic Stern-Gerlach Experiment from Electron Diffraction

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    Using the wave nature of the electrons, we demonstrate that a transverse spin current can be generated simply by the diffraction through a single slit in the spin-orbital coupling system of the two-dimensional electron gas. The diffracted electron picks up the transverse momentum. The up spin electron goes one way and the down spin electron goes the other, producing the coherent spin current. In the system of spin-orbital coupling 1013\sim10^{-13} eV\cdotm, the \emph{out-of-plane} component of the spin of the electron can be generated up to 0.42 \hbar. Based on this effect, a novel device of grating to distill spin is designed. Two first diffraction peaks of electron carry different spins, duplicating the non-magnetic version of Stern-Gerlach experiment. The direction of the spin current can be controlled by the gate voltage with low energy cost.Comment: 4 pages, 4 figure

    Existence of translating solutions to the flow by powers of mean curvature on unbounded domains

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    In this paper, we prove the existence of classical solutions of the Dirichlet problem for a class of quasi-linear elliptic equations on unbounded domains like a cone or a U-type domain. This problem comes from the study of mean curvature flow and its generalization, the flow by powers of mean curvature. Our approach is a modified version of the classical Perron method, where the solutions to the minimal surface equation are used as sub-solutions and a family auxiliary functions are constructed as super-solutions.Comment: 30 page

    Hidden charm pentaquark and Λ(1405)\Lambda(1405) in the Λb0ηcKp(πΣ)\Lambda^0_b \to \eta_c K^- p (\pi \Sigma) reaction

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    We have performed a study of the Λb0ηcKp\Lambda^0_b \to \eta_c K^- p and Λb0ηcπΣ\Lambda^0_b \to \eta_c \pi \Sigma reactions based on the dominant Cabibbo favored weak decay mechanism. We show that the KpK^- p produced only couples to Λ\Lambda^* states, not Σ\Sigma^* and that the πΣ\pi \Sigma state is only generated from final state interaction of KˉN\bar{K}N and ηΛ\eta \Lambda channels which are produced in a primary stage. This guarantees that the πΣ\pi \Sigma state is generated in isospin I=0I=0 and we see that the invariant mass produces a clean signal for the Λ(1405)\Lambda(1405) of higher mass at 14201420 MeV. We also study the ηcp\eta_c p final state interaction, which is driven by the excitation of a hidden charm resonance predicted before. We relate the strength of the different invariant mass distributions and find similar strengths that should be clearly visible in an ongoing LHCb experiment. In particular we predict that a clean peak should be seen for a hidden charm resonance that couples to the ηcp\eta_c p channel in the invariant ηcp\eta_c p mass distribution.Comment: 8 pages, 7 figure

    Bˉ0\bar B^0, BB^- and Bˉs0\bar B^0_s decays into J/ψJ/\psi and KKˉK \bar K or πη\pi \eta

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    We study the Bˉs0J/ψK+K\bar B^0_s \to J/\psi K^+ K^-, Bˉ0J/ψK+K\bar B^0 \to J/\psi K^+ K^-, BJ/ψK0KB^- \to J/\psi K^0 K^-, Bˉ0J/ψπ0η\bar B^0 \to J/\psi \pi^0 \eta and BJ/ψπηB^- \to J/\psi \pi^- \eta decays and compare their mass distributions with those obtained for the Bˉs0J/ψπ+π\bar B^0_s \to J/\psi \pi^+ \pi^- and Bˉ0J/ψπ+π\bar B^0 \to J/\psi \pi^+ \pi^-. The approach followed consist in a factorization of the weak part and the hadronization part into a factor which is common to all the processes. Then what makes the reactions different are some trivial Cabibbo-Kobayashi-Maskawa matrix elements and the weight by which the different pairs of mesons appear in a primary step plus their final state interaction. These elements are part of the theory and thus, up to a global normalization factor, all the invariant mass distributions are predicted with no free parameters. Comparison is made with the limited experimental information available. Further comparison of these results with coming LHCb measurements will be very valuable to make progress in our understanding of the meson-meson interaction and the nature of the low lying scalar meson resonances, f0(500),f0(980)f_0(500), f_0(980) and a0(980)a_0(980).Comment: 12 pages, 6 figures; v2: discussion added, references added, final version published in EPJ
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