151,053 research outputs found

    Oscillatory instability of radiative shocks with multiple cooling processes

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    The stand-off shock formed in the accretion flow on to a stationary wall, such as the surface of a white dwarf, may be thermally unstable, depending on the cooling processes which dominate the post-shock flow. Some processes lead to instability, while others tend to stabilize the shock. We consider competition between the destabilizing influence of thermal bremsstrahlung cooling, and a stabilizing process which is a power law in density and temperature. Cyclotron cooling and processes which are of order 1, 3/2 and 2 in density are considered. The relative efficiency and power-law indices of the second mechanism are varied, and particular effects on the stability properties and frequencies of oscillation modes are examined

    Giant isotope effect and spin state transition induced by oxygen isotope exchange in (Pr1βˆ’xSmx)0.7Ca0.3CoO3Pr_{1-x}Sm_x)_{0.7}Ca_{0.3}CoO_3

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    We systematically investigate effect of oxygen isotope in (Pr1βˆ’xSmx)0.7Ca0.3CoO3(Pr_{1-x}Sm_x)_{0.7}Ca_{0.3}CoO_3 which shows a crossover with x from ferromagnetic metal to the insulator with spin-state transition. A striking feature is that effect of oxygen isotope on the ferromagnetic transition is negligible in the metallic phase, while replacing 16O^{16}O with 18O^{18}O leads to a giant up-shift of the spin-state transition temperature (TsT_s) in the insulating phase, especially TsT_s shifts from 36 to 54 K with isotope component Ξ±S=βˆ’4.7\alpha_S=-4.7 for the sample with x=0.175. A metal-insulator transition is induced by oxygen isotope exchange in the sample x=0.172 being close to the insulating phase. The contrasting behaviors observed in the two phases can be well explained by occurrence of static Jahn-Teller distortions in the insulating phase, while absence of them in the metallic phase.Comment: 4 pages, 5 figure

    Intrinsic electron-doping in nominal "non-doped" superconducting (La,Y)2_2CuO4_4 thin films grown by dc magnetron sputtering

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    The superconducting nominal "non-doped" La1.85Y0.15CuO4La_{1.85}Y_{0.15}CuO_4 (LYCO) thin films are successfully prepared by dc magnetron-sputtering and in situ post-annealing in vacuum. The best TC0T_{C0} more than 13K is achieved in the optimal LYCO films with highly pure c-axis oriented T'-type structure. In the normal state, the quasi-quadratic temperature dependence of resistivity, the negative Hall coefficient and effect of oxygen content in the films are quite similar to the typical Ce-doped T'-214 cuprates, suggesting that T'-LYCO shows the electron-doping nature like known n-type cuprates, and is not a band superconductor as proposed previously. The charge carriers are considered to be induced by oxygen deficiency.Comment: 5 pages, 7 figure

    Thermodynamic properties of Ba1-xMxFe2As2 (M = La and K)

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    The specific heat C(T)C(T) of BaFe2_2As2_2 single crystal, electron-doped Ba0.7_{0.7}La0.3_{0.3}Fe2_2As2_2 and hole-doped Ba0.5_{0.5}K0.5_{0.5}Fe2_2As2_2 polycrystals were measured. For undoped BaFe2_2As2_2 single crystal, a very sharp specific heat peak was observed at 136 K. This is attributed to the structural and antiferromagnetic transitions occurring at the same temperature. C(T)C(T) of the electron-doped non-superconducting Ba0.7_{0.7}La0.3_{0.3}Fe2_2As2_2 also shows a small peak at 120 K, indicating a similar but weaker structural/antiferromagnetic transition. For the hole-doped superconducting Ba0.5_{0.5}K0.5_{0.5}Fe2_2As2_2, a clear peak of C/TC/T was observed at TcT_c = 36 K, which is the highest peak seen at superconducting transition for iron-based high-TcT_c superconductors so far. The electronic specific heat coefficient γ\gamma and Debye temperature ΘD\Theta_D of these compounds were obtained from the low temperature data

    Origin of superconductivity in nominally "undoped" T'-La2βˆ’x_{2-x}Yx_{x}CuO4_{4} films

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    We have systematically studied the transport properties of the La2βˆ’x_{2-x}Yx_{x}CuO4_{4}(LYCO) films of T'-phase (0.05≀x≀0.300.05\leq x \leq 0.30). In this nominally "undoped" system, superconductivity was acquired in certain Y doping range (0.10≀x≀0.200.10\leq x \leq 0.20). Measurements of resistivity, Hall coefficients in normal states and resistive critical field (Hc2ρH^\rho_{c2})in superconducting states of the T'-LYCO films show the similar behavior as the known Ce-doped n-type cuprate superconductors, indicating the intrinsic electron-doping nature. The charge carriers are induced by oxygen deficiency. Non-superconducting Y-doped Pr- or Nd-based T'-phase cuprate films were also investigated for comparison, suggesting the crucial role of the radii of A-site cations in the origin of superconductivity in the nominally "undoped" cuptates. Based on a reasonable scenario in the microscopic reduction process, we put forward a self-consistent interpretation of these experimental observations.Comment: 8 pages, 9 figure

    Novel dynamical effects and glassy response in strongly correlated electronic system

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    We find an unconventional nucleation of low temperature paramagnetic metal (PMM) phase with monoclinic structure from the matrix of high-temperature antiferromagnetic insulator (AFI) phase with tetragonal structure in strongly correlated electronic system BaCo0.9Ni0.1S1.97BaCo_{0.9}Ni_{0.1}S_{1.97}. Such unconventional nucleation leads to a decease in resistivity by several orders with relaxation at a fixed temperature without external perturbation. The novel dynamical process could arise from the competition of strain fields, Coulomb interactions, magnetic correlations and disorders. Such competition may frustrate the nucleation, giving rise to a slow, nonexponential relaxation and "physical aging" behavior.Comment: 5 pages, 4 figure
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