113,469 research outputs found

    Magnetic field dependence of electronic properties of MoS2_2 quantum dots with different edges

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    Using the tight-binding approach, we investigate the energy spectrum of square, triangular and hexagonal MoS2_2 quantum dots (QDs) in the presence of a perpendicular magnetic field. Novel edge states emerge in MoS2_2 QDs, which are distributed over the whole edge which we call ring states. The ring states are robust in the presence of spin-orbit coupling (SOC). The corresponding energy levels of the ring states oscillate as function of the perpendicular magnetic field which are related to Aharonov-Bohm oscillations. Oscillations in the magnetic field dependence of the energy levels and the peaks in the magneto-optical spectrum emerge (disappear) as the ring states are formed (collapsed). The period and the amplitude of the oscillation decreases with the size of the MoS2_2 QDs.Comment: 11 pages, 9 figures, Accepted by Phys. Rev.

    Out of plane effect on the superconductivity of Sr2-xBaxCuO3+y with Tc up to 98K

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    A series of new Sr2-xBaxCuO3+y (0 x 0.6) superconductors were prepared using high-pressure and high-temperature synthesis. A Rietveld refinement based on powder x-ray diffraction confirms that the superconductors crystallize in the K2NiF4-type structure of a space group I4/mmm similar to that of La2CuO4 but with partially occupied apical oxygen sites. It is found that the superconducting transition temperature Tc of this Ba substituted Sr2CuO3+y superconductor with constant carrier doping level, i.e., constant d, is controlled not only by order/disorder of apical-O atoms but also by Ba content. Tcmax =98 K is achieved in the material with x=0.6 that reaches the record value of Tc among the single-layer copper oxide superconductors, and is higher than Tc=95K of Sr2CuO3+y with optimally ordered apical-O atoms. There is Sr-site disorder in Sr2-xBaxCuO3+y which might lead to a reduction of Tc. The result indicates that another effect surpasses the disorder effect that is related either to the increased in-plane Cu-O bond length or to elongated apical-O distance due to Ba substitution with larger cation size. The present experiment demonstrates that the optimization of local geometry out of the Cu-O plane can dramatically enhance Tc in the cuprate superconductors.Comment: 23 Pages, 1 Table, 5 Figure

    Five-quark components in Δ(1232)Nπ\Delta(1232)\to N\pi decay

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    Five-quark qqqqqˉqqqq\bar q components in the Δ(1232)\Delta(1232) are shown to contribute significantly to Δ(1232)Nπ\Delta(1232)\to N\pi decay through quark-antiquark annihilation transitions. These involve the overlap between the qqqqqq and qqqqqˉqqqq\bar q components and may be triggered by the confining interaction between the quarks. With a \sim 10% admixture of five-quark components in the Δ(1232)\Delta(1232) the decay width can be larger by factors 2 - 3 over that calculated in the quark model with 3 valence quarks, depending on the details of the confining interaction. The effect of transitions between the qqqqqˉqqqq\bar q components themselves on the calculated decay width is however small. The large contribution of the quark-antiquark annihilation transitions thus may compensate the underprediction of the width of the Δ(1232)\Delta(1232) by the valence quark model, once the Δ(1232)\Delta(1232) contains qqqqqˉqqqq\bar q components with \sim 10% probability.Comment: accepted versio

    Diamagnetism around the Meissner transition in a homogeneous cuprate single crystal

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    The in-plane diamagnetism around the Meissner transition was measured in a Tl2_2Ba2_2Ca2_2Cu3_3O10_{10} single crystal of high chemical and structural quality, which minimizes the inhomogeneity and disorder rounding effects on the magnetization. When analyzed quantitatively and consistently above and below the transition in terms of the Ginzburg-Landau (GL) approach with fluctuations of Cooper pairs and vortices, these data provide a further confirmation that the observed Meissner transition is a conventional GL superconducting transition in a homogeneous layered superconductor.Comment: 5 pages, including 3 figure
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