13,217 research outputs found

    Anomalous Josephson Effect in magnetic Josephson junctions with noncentrosymmetric superconductors

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    We show that the two-band nature of noncentrosymmetric superconductors leads naturally to an anomalous Josephson current appearing at zero phase difference in a clean noncentrosymmetric superconductor/ferromagnet/noncentrosymmetric superconductor junction. The two-band nature provides two sets of Andreev bound states which carry two supercurrents with different amplitudes. When the magnetization direction of the ferromagnet is suitably chosen, two supercurrents experience opposite phase shifts from the conventional sinusoidal current-phase relation. Then the total Josephson current results in a continuously tunable ground-state phase difference by adjusting the ferromagnet parameters and the triplet-singlet ratio of noncentrosymmetric superconductors. The physics picture and analytical results are given on the basis of the ss+pp wave, while the numerical results are reported on both ss+pp and dd+pp waves. For the dd+pp wave, we find novel states in which the supercurrents are totally carried by continuous propagating states instead of discrete Andreev bound states. Instead of carrying supercurrent, the Andreev bound states which here only appear above the Fermi energy block the supercurrent flowing along the opposite direction. These novel states advance the understaning of the relation between Andreev bound states and the Josephson current. And the ground-state phase difference serves as a tool to determine the triplet-singlet ratio of noncentrosymmetric superconductors.Comment: 10pages, 6figure

    Neutrinos from gamma-ray bursts: propagation of cosmic rays in their host galaxies

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    Gamma-ray bursts (GRBs) are proposed as candidate sources of ultra-high energy cosmic rays (UHECRs). We study the possibility that the PeV neutrinos recently observed by IceCube are produced by GRB cosmic rays interacting with the interstellar gas in the host galaxies. By studying the relation between the X-ray absorption column density N_H and the surface star-formation rate of GRB host galaxies, we find that N_H is a good indicator of the surface gas density of the host galaxies. Then we are able to calculate the neutrino production efficiency of CRs for GRBs with known N_H. We collect a sample of GRBs that have both measurements of N_H and accurate gamma-ray fluence, and attempt to calculate the accumulated neutrino flux based on the current knowledge about GRBs and their host galaxies. When the CR intensity produced by GRBs is normalized with the observed UHECR flux above 1019eV10^{19}{\rm eV}, the accumulated neutrino flux at PeV energies is estimated to be about (0.3Β±0.2)Γ—10βˆ’8GeVΒ cmβˆ’2Β sβˆ’1Β srβˆ’1(0.3\pm0.2)\times10^{-8} \rm{GeV\ cm^{-2}\ s^{-1}\ sr^{-1}} (per flavor) under the assumption that GRB energy production rate follows the cosmic star-formation rate and the favorable assumption about the CR diffusion coefficient. This flux is insufficient to account for the IceCube observations, but the estimate suffers from some assumptions in the calculation and thus we can not rule out this scenario at present.Comment: 8 pages, 3 figures, 2 tables, to appear in ApJ

    Self-similar subsets of the Cantor set

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    In this paper, we study the following question raised by Mattila in 1998: what are the self-similar subsets of the middle-third Cantor set \C? We give criteria for a complete classification of all such subsets. We show that for any self-similar subset \F of \C containing more than one point every linear generating IFS of \F must consist of similitudes with contraction ratios Β±3βˆ’n\pm 3^{-n}, n∈Nn\in \N. In particular, a simple criterion is formulated to characterize self-similar subsets of \C with equal contraction ratio in modulus

    Electrically modulated SQUID with single Josephson junction coupled by a time-reversal breaking Weyl semimetal thin film

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    Usually, the superconducting quantum interference device (SQUID) consists of two Josephson junctions and the interference therein is modulated by a magnetic flux. In this work, we propose an electrically modulated SQUID consisting of single Josephson junction coupled by a time-reversal breaking Weyl semimetal thin film. For a low Fermi energy, the Josephson current is only mediated by Fermi arc surface states, and has an arbitrary ground-state phase difference \phi0 which is directly proportional to the product of the transverse electric field and the cross section area of the junction.For a suitable Fermi energy, the bulk states make comparable contributions to the Josephson current with the current-phase relation of a 0-junction. The interference between the surface channel and the bulk channel results in an electrically modulated SQUID with single Josephson junction, which provides an experimental proposal to identify magnetic Weyl semimetals and may have potential applications in superconducting quantum computation.Comment: 5 figure

    Neural method for Explicit Mapping of Quasi-curvature Locally Linear Embedding in image retrieval

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    This paper proposed a new explicit nonlinear dimensionality reduction using neural networks for image retrieval tasks. We first proposed a Quasi-curvature Locally Linear Embedding (QLLE) for training set. QLLE guarantees the linear criterion in neighborhood of each sample. Then, a neural method (NM) is proposed for out-of-sample problem. Combining QLLE and NM, we provide a explicit nonlinear dimensionality reduction approach for efficient image retrieval. The experimental results in three benchmark datasets illustrate that our method can get better performance than other state-of-the-art out-of-sample methods

    Full pseudoscalar mesonic chiral Lagrangian at p6 order under the unitary group

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    We construct the full p6 order chiral Lagrangians for the unitary group and special unitary groups, including nf-, three- and two-flavor cases, all bilinear currents (scalar, pseudoscalar, vector, axial-vector and tensor currents) and theta parameter. The number of independent operators are 1391, 1326 and 969 for each of the flavor unitary groups. From these results, we find one extra linear relation among the traditional p4 order low-energy constants under the U(3) group, and some more linear relations with tensor sources for the p6 order low-energy constants in the special unitary groups. We develop a scheme to obtain the relations for the dependent operators in terms of independent operators.Comment: 23 page

    Hadronization effects on the baryon-strangeness correlation in quark combination models

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    The baryon-strangeness correlation in the hadronization of the quark matter is studied within the quark combination mechanism. We calculate the correlation coefficient CBS=βˆ’3(⟨BSβŸ©βˆ’βŸ¨B⟩⟨S⟩)/(⟨S2βŸ©βˆ’βŸ¨S⟩2)C_{BS} = -3\big(\langle B S \rangle -\langle B\rangle \langle S\rangle\big)/\big( \langle S^2 \rangle-\langle S \rangle^2 \big) of initial hadrons produced from the deconfined free quark system with CBS(q)=1C^{(q)}_{BS}=1. The competition of the production of baryons against that of mesons is the key dynamics that is most relevant to the change of baryon-strangeness correlation during system hadronization. Results of quark combination under the Poisson statistics agree with the statistical model predictions for a hadron resonance gas at vanishing chemical potential but differ from those at relatively large chemical potentials. Results beyond Poisson statistics are also obtained and are compared with calculations of Lattice QCD in the phase boundary, giving the best agreement at temperature T=163T =163 MeV. We predict the dependence of the CBSC_{BS} of hadron system on the baryon chemical potential and strangeness. These predictions are expected to be tested by the future Lattice QCD calculations at non-zero chemical potentials and/or by the Beam Energy Scan experiment of STAR Collaboration at RHIC.Comment: 10 pages, 6 figure

    Enhanced magneto-optical response due to the flat band in nanoribbons made from the Ξ±βˆ’T3\alpha-T_3 lattice

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    We study the optical response of nanoribbons made from the Ξ±βˆ’T3\alpha-T_3 lattice under a weak magnetic field in the terahertz to far-infrared regime. It is found that the magnetic field can open a gap in the band structure and induce a new absorption peak with much reduced frequency in metallic armchair ribbons and a class of zigzag ribbons with particular boundaries. This tunable magneto-optical modulation effect is attributed to the interband transitions between the flat band and the propagating bands. By contrast, this magnetic modulation of gap opening and optical conductance is much weaker in metallic armchair graphene ribbons (the case of Ξ±=0\alpha=0) in which the flat band is absent. The enhancement in the Ξ±βˆ’T3\alpha-T_3 model is analytically investigated and explained within the perturbation theory for metallic armchair ribbons. The magnetic field induced valley degeneracy lifting and valley splitting of the absorption peak are also discussed in the case of zigzag ribbons. These findings pave the way for magneto-optics devices based on the Ξ±βˆ’T3\alpha-T_3 model materials.Comment: 7 pages, 7 figures; accepted by Physical Review

    SU(2) Charges as Angular-momentum in N=1 Self-dual Supergravity

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    The N=1 self-dual supergravity has SL(2.C) symmetry. This symmetry results in SU(2) charges as the angular-momentum. As in the non-supersymmetric self-dual gravity, the currents are also of their potentials and are therefore identically conserved. The charges are generally invariant and gauge covariant under local SU(2) transforms approaching to be rigid at spatial infinity. The Poisson brackets constitute su(2) algebra and hence can be interpreted as the generally covariant conservative angular-momentum.Comment: 8 pages, Latex, no figures, to appear in Int. J. Theor. Phy

    Numerical study of the quantum valley Hall effect

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    Under more consideration, it seems that bulk valley current mediated nonlocal resistance is inconsistent with Landau-Buttiker formalism. We believe Landau-Buttiker formalism is right and the declared bulk valley current mediated nonlocal resistance is questionable and the experimental signal should be attributed to other origins.Comment: It seems that bulk valley current mediated nonlocal resistance is nconsistent with Landau-Buttiker formalis
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