8,261 research outputs found

    Strain induced magnetic domain evolution and spin re-orientation transition in epitaxial manganite films

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    The evolution of magnetic domain structure in epitaxial La0.625_{0.625}Ca0.375_{0.375}MnO3_3 films on (001) NdGaO3_3 is monitored as a function of temperature and magnetic field using Magnetic Force Microscopy. We see two distinct regions of magnetic orientational order; one in-plane displaying contrast-less image and the other tilted away from the film plane forming a distinct stripe pattern. A strong domain splitting is observed at the boundary of two regions, which is resilient to reorientation with temperature and magnetic field. We propose a model magnetic free energy functional to explain the mechanism of domain splitting seen in manganite films

    Electronic reconstruction and enhanced superconductivity at La1.6x_{1.6-x}Nd0.4_{0.4}Srx_{x}CuO4_{4}/La1.55_{1.55}Sr0.45_{0.45}CuO4_{4} bilayer interface

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    We report enhanced superconductivity in bilayer thin films consisting of superconducting La1.6x_{1.6-x}Nd0.4_{0.4}Srx_{x}CuO4_{4} with 0.06 x<\leq x< 0.20 and metallic but non-superconducting La1.55_{1.55}Sr0.45_{0.45}CuO4_{4}. These bilayers show a maximum increase in superconducting transition temperature (TcT_c) of more than 200% for xx = 0.06 while no change in TcT_c is observed for the bilayers with xx\geq 0.20. The analysis of the critical current and kinetic inductance data suggests 2-3 unit cells thick interfacial layer electronically perturbed to have a higher TcT_c. A simple charge transfer model with cation intermixing explains the observed TcT_c in bilayers. Still the unusually large thickness of interfacial superconducting layers can not be explained in terms of this model. We believe the stripe relaxation as well as the proximity effect also influence the superconductivity of the interface

    Changes in the electronic structure and properties of graphene induced by molecular charge-transfer

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    Interaction with electron donor and acceptor molecules such as aniline and nitrobenzene brings about marked changes in the Raman spectrum and the electronic structure of graphene, prepared by the exfoliation of graphitic oxide.Comment: 13 pages, 4 figure

    Two-dimensional electron-gas-like charge transport at magnetic Heusler alloy-SrTiO3_3 interface

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    We report remarkably low residual resistivity, giant residual resistivity ratio, free-electron-like Hall resistivity and high mobility (\approx 104^4 cm2^2V1^{-1}s1^{-1}) charge transport in epitaxial films of Co2_2MnSi and Co2_2FeSi grown on (001) SrTiO3_3. This unusual behavior is not observed in films deposited on other cubic oxide substrates of comparable lattice parameters. The scaling of the resistivity with thickness of the films allow extraction of interface conductance, which can be attributed to a layer of oxygen vacancies confined within 1.9 nm of the interface as revealed by atomically resolved electron microscopy and spectroscopy. The high mobility transport observed here at the interface of a fully spin polarized metal is potentially important for spintronics applications

    Interface superconductivity in La1.48_{1.48}Nd0.4_{0.4}Sr0.12_{0.12}CuO4_{4}/La1.84_{1.84}Sr0.16_{0.16}CuO4_{4} bilayers

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    We identify a distinct superconducting phase at the interface of a La1.48_{1.48}Nd0.4_{0.4}Sr0.12_{0.12}CuO4_4 (LNSCO)/La1.84_{1.84}Sr0.16_{0.16}CuO4_4 (LSCO) epitaxial bilayer system using ac screening measurements. A model based on inter-diffusion of quasiparticles and condensate at the interface yields a thickness of \sim 25 nm for the interfacial layer. Two-dimensional superconductivity of the interface layer appears to be governed by Kosterlitz-Thouless-Berezinskii transition. A parallel magnetic field suppresses the superconducting transition temperature of this layer with a pair breaking parameter α\alpha varying as H2H^2

    Fast protocol for high frequency in vitro cloning of Banana (Musa acuminata) cv. Grande Naine

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    An investigation was conducted on Fast Protocol for High Frequency in vitro cloning of Banana (Musa acuminata) cv. Grande Naine at the Biotechnology-cum-Tissue Culture Center, OUAT, Bhubaneswar, during the year 2012. This has helped to determine the best media compositions for shoot multiplication and rooting of cv. Grande Naine, so as to get optimum results with a minimized cost of production. MS medium supplemented with 4.0 mg/1 Benzylaminopurine (BAP) and 2.0 mg/1 Kinetin gave the highest number of shoot/explants (11.33) in 30 days. However, MS medium when supplemented with 6.0 mg/1 BAP produced a maximum number of leaves (19.07) with a maximum height 2.73 cm. Among various concentrations of indole-3-acetic acid (IAA), indole-3-butyric acid (IBA) and naphthaleneacetic acid (NAA) for rooting. Half MS medium supplemented with 1.0 mg/1 IBA was found to be ideal for early rooting and producing more number of roots in 21 days. However, MS basal medium was found to be the best treatment to support the formation of long roots. This protocol can be very useful to the future research worker and as well as entrepreneurs for mass production of banana (Musa acuminata) cv. Grande Naine

    Structure and Rheology of the Defect-gel States of Pure and Particle-dispersed Lyotropic Lamellar Phases

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    We present important new results from light-microscopy and rheometry on a moderately concentrated lyotropic smectic, with and without particulate additives. Shear-treatment aligns the phase rapidly, except for a striking network of oily-streak defects, which anneals out much more slowly. If spherical particles several microns in diameter are dispersed in the lamellar medium, part of the defect network persists under shear-treatment, its nodes anchored on the particles. The sample as prepared has substantial storage and loss moduli, both of which decrease steadily under shear-treatment. Adding particles enhances the moduli and retards their decay under shear. The data for the frequency-dependent storage modulus after various durations of shear-treatment can be scaled to collapse onto a single curve. The elasticity and dissipation in these samples thus arises mainly from the defect network, not directly from the smectic elasticity and hydrodynamics.Comment: 19 pages inclusive of 12 PostScript figures, uses revtex, psfrag and epsfig. Revised version, accepted for publication in Euro. Phys. J. B, with improved images of defect structure and theoretical estimates of network elasticity and scalin
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