956 research outputs found

    Temperature- and magnetic-field-dependent resistivity of MgB2 sintered at high temperature and high pressure condition

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    We report the temperature- and magnetic-field-dependent resistivity of MgB2 sintered at high temperature and high pressure condition. The superconducting transition width for the resistivity measurement was about 0.4 K, and the low-field magnetization showed a sharp superconducting transition with a transition width of about 1 K. The resistivity in the normal state roughly followed T^2 behavior with smaller residual resistivity ratio (RRR) of 3 over broad temperature region above 100 K rather than reported T^3 behavior with larger RRR value of ~ 20 in the samples made at lower pressures. Also, the resistivity did not change appreciably with the applied magnetic field, which was different from previous report. These differences were discussed with the microscopic and structural change due to the high-pressure sintering.Comment: 2 pages, 3 figures. Accepted by Physica

    Spin Fluctuation Induced Dephasing in a Mesoscopic Ring

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    We investigate the persistent current in a hybrid Aharonov-Bohm ring - quantum dot system coupled to a reservoir which provides spin fluctuations. It is shown that the spin exchange interaction between the quantum dot and the reservoir induces dephasing in the absence of direct charge transfer. We demonstrate an anomalous nature of this spin-fluctuation induced dephasing which tends to enhance the persistent current. We explain our result in terms of the separation of the spin from the charge degree of freedom. The nature of the spin fluctuation induced dephasing is analyzed in detail.Comment: 4 pages, 4 figure

    Effect of Charge Fluctuations on the Persistent Current through a Quantum Dot

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    We study coherent charge transfer between an Aharonov-Bohm ring and a side-attached quantum dot. The charge fluctuation between the two sub-structures is shown to give rise to algebraic suppression of the persistent current circulating the ring as the size of the ring becomes relatively large. The charge fluctuation at resonance provides transition between the diamagnetic and the paramagnetic states. Universal scaling, crossover behavior of the persistent current from a continuous to a discrete energy limit in the ring is also discussed.Comment: 5 pages, 4 figure

    Tau-Sleptons and Tau-Sneutrino in the MSSM with Complex Parameters

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    We present a phenomenological study of tau-sleptons stau_1,2 and tau-sneutrino in the Minimal Supersymmetric Standard Model with complex parameters A_tau, mu and M_1. We analyse production and decays of stau_1,2 and tau-sneutrino at a future e^+ e^- collider. We present numerical predictions for the important decay rates, paying particular attention to their dependence on the complex parameters. The branching ratios of the fermionic decays of stau_1 and tau-sneutrino show a significant phase dependence for tan(beta) < 10. For tan(beta) > 10 the branching ratios for the stau_2 decays into Higgs bosons depend very sensitively on the phases. We show how information on the phase phi(A_tau) and the other fundamental stau parameters can be obtained from measurements of the stau masses, polarized cross sections and bosonic and fermionic decay branching ratios, for small and large tan(beta) values. We estimate the expected errors for these parameters. Given favorable conditions, the error of A_tau is about 10% to 20%, while the errors of the remaining stau parameters are in the range of approximately 1% to 3%. We also show that the induced electric dipole moment of the tau-lepton is well below the current experimental limit.Comment: LaTex, 25 pages, 11 figures (included); v2: extended discussion on error determination, version to appear in Phys.Rev.

    Beam Dynamics of Qi Storage Rings

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    This research was sponsored by the National Science Foundation Grant NSF PHY-931478

    Characterization, identification, and cloning of the S-layer protein from Cytophaga sp

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    We characterized, identified, and cloned a major protein which comprised 16% of the total proteins from Cytophaga sp. cell lysate. After French pressing, the fraction of cell envelope was treated with 0.2% Triton X-100 to remove cell membranes. Subsequent SDS-PAGE analysis of the Triton X-100-insoluble cell wall revealed a protein of 120 kDa with a pI of 5.4, which was identified by gold immunostaining as the surface (S)-layer protein of this soil bacterium. The nucleotide sequence of the cloned S-layer protein gene (slp) encoding this protein consisted of 3144 nucleotides with an ORF for 1047 amino acids, which included a typical 32-amino acid leader peptide sequence. Amino acid sequence alignment revealed 29-48% similarity between this protein and the S-layer proteins from other prokaryotic organisms. The 120-kDa protein from the Cytophaga sp. cell lysate has been characterized as a member of the S-layer proteins, and the slp gene was cloned and expressed in Escherichia coli. E. coli harboring the plasmid containing the 600- or 800-bp DNA fragment upstream of the initiation codon of the slp gene, in the presence of the reporter gene rsda (raw starch digesting amylase), showed amylase activity in starch containing plate. The putative promoter region of slp located 600 bp upstream of the initiation codon might be used for foreign gene expression

    Anti-Kondo resonance in transport through a quantum wire with a side-coupled quantum dot

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    An interacting quantum dot side-coupled to a perfect quantum wire is studied. Transport through the quantum wire is investigated by using an exact sum rule and the slave-boson mean field treatment. It is shown that the Kondo effect provides a suppression of the transmission due to the destructive interference of the ballistic channel and the Kondo channel. At finite temperatures, anti-resonance behavior is found as a function of the quantum dot level position, which is interpreted as a crossover from the high temperature Kondo phase to the low temperature charge fluctuation phase.Comment: 4 pages Revtex, 3 eps figure

    Neutrino Oscillations and Collider Test of the R-parity Violating Minimal Supergravity Model

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    We study the R-parity violating minimal supergravity models accounting for the observed neutrino masses and mixing, which can be tested in future collider experiments. The bi-large mixing can be explained by allowing five dominant tri-linear couplings λ1,2,3 \lambda'_{1,2,3} and λ1,2\lambda_{1,2}. The desired ratio of the atmospheric and solar neutrino mass-squared differences can be obtained in a very limited parameter space where the tree-level contribution is tuned to be suppressed. In this allowed region, we quantify the correlation between the three neutrino mixing angles and the tri-linear R-parity violating couplings. Qualitatively, the relations λ1<λ2λ3| \lambda'_1 | < | \lambda'_2| \sim | \lambda'_3|, and λ1λ2|\lambda_1| \sim |\lambda_2| are required by the large atmospheric neutrino mixing angle θ23\theta_{23} and the small angle θ13\theta_{13}, and the large solar neutrino mixing angle θ12\theta_{12}, respectively. Such a prediction on the couplings can be tested in the next linear colliders by observing the branching ratios of the lightest supersymmetric particle (LSP). For the stau or the neutralino LSP, the ratio λ12:λ22:λ12+λ22|\lambda_1|^2: |\lambda_2|^2: |\lambda_1|^2 + |\lambda_2|^2 can be measured by establishing Br(eν):Br(μν):Br(τν)Br(e\nu): Br(\mu\nu) : Br(\tau\nu) or Br(νe±τ):Br(νμ±τ):Br(ντ±τ)Br(\nu e^\pm \tau^\mp ): Br(\nu\mu^\pm\tau^\mp) : Br(\nu\tau^\pm\tau^\mp), respectively. The information on the couplings λi\lambda'_i can be drawn by measuring Br(litbˉ)λi2Br(l_i t \bar{b}) \propto |\lambda'_i|^2 if the neutralino LSP is heavier than the top quark.Comment: RevTex, 25 pages, 8 eps figure

    Enhancement of service life of polymer electrolyte fuel cells through application of nanodispersed ionomer

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    Copyright © 2020 The Authors, some rights reserved.In polymer electrolyte fuel cells (PEFCs), protons from the anode are transferred to the cathode through the ionomer membrane. By impregnating the ionomer into the electrodes, proton pathways are extended and high proton transfer efficiency can be achieved. Because the impregnated ionomer mechanically binds the catalysts within the electrode, the ionomer is also called a binder. To yield good electrochemical performance, the binder should be homogeneously dispersed in the electrode and maintain stable interfaces with other catalyst components and the membrane. However, conventional binder materials do not have good dispersion properties. In this study, a facile approach based on using a supercritical fluid is introduced to prepare a homogeneous nanoscale dispersion of the binder material in aqueous alcohol. The prepared binder exhibited high dispersion characteristics, crystallinity, and proton conductivity. High performance and durability were confirmed when the binder material was applied to a PEFC cathode electrode11sciescopu
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