98,088 research outputs found

    Onset of unsteady horizontal convection in rectangle tank at Pr=1Pr=1

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    The horizontal convection within a rectangle tank is numerically simulated. The flow is found to be unsteady at high Rayleigh numbers. There is a Hopf bifurcation of RaRa from steady solutions to periodic solutions, and the critical Rayleigh number RacRa_c is obtained as Rac=5.5377×108Ra_c=5.5377\times 10^8 for the middle plume forcing at Pr=1Pr=1, which is much larger than the formerly obtained value. Besides, the unstable perturbations are always generated from the central jet, which implies that the onset of instability is due to velocity shear (shear instability) other than thermally dynamics (thermal instability). Finally, Paparella and Young's [J. Fluid Mech. 466 (2002) 205] first hypotheses about the destabilization of the flow is numerically proved, i.e. the middle plume forcing can lead to a destabilization of the flow.Comment: 4pages, 6 figures, extension of Chin. Phys. Lett. 2008, 25(6), in pres

    Phonon anomalies in pure and underdoped R{1-x}K{x}Fe{2}As{2} (R = Ba, Sr) investigated by Raman light scattering

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    We present a detailed temperature dependent Raman light scattering study of optical phonons in Ba{1-x}K{x}Fe{2}As{2} (x ~ 0.28, superconducting Tc ~ 29 K), Sr{1-x}K{x}Fe{2}As{2} (x ~ 0.15, Tc ~ 29 K) and non-superconducting BaFe{2}As{2} single crystals. In all samples we observe a strong continuous narrowing of the Raman-active Fe and As vibrations upon cooling below the spin-density-wave transition Ts. We attribute this effect to the opening of the spin-density-wave gap. The electron-phonon linewidths inferred from these data greatly exceed the predictions of ab-initio density functional calculations without spin polarization, which may imply that local magnetic moments survive well above Ts. A first-order structural transition accompanying the spin-density-wave transition induces discontinuous jumps in the phonon frequencies. These anomalies are increasingly suppressed for higher potassium concentrations. We also observe subtle phonon anomalies at the superconducting transition temperature Tc, with a behavior qualitatively similar to that in the cuprate superconductors.Comment: 5 pages, 6 figures, accepted versio

    Application of the 'ESCIMO' theory to turbulent diffusion flames

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    Effect of cadmium hyperaccumulation on antioxidative defense and proline accumulation of Solanum nigrum

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    Changes in cadmium (Cd) accumulation, the activity of antioxidant enzymes including superoxide dismutase (SOD), peroxidase (POD), catalase (CAT) and the concentrations of malondialdehyde (MDA), chlorophyll and free proline in Solanum nigrum, Cd-hyperaccumulator were examined and compared with a non-hyperaccumulator, Solanum lycopersicum L. It was indicated that the root and leaf SOD, POD and CAT activities of S. nigrum were significantly higher than that of S. lycopersicum. In comparison with S. nigrum, there was a decrease in the growth and chlorophyll content, and an increase in MDA concentrations in the roots and leaves of S. lycopersicum. Although lipid peroxidation was promoted in both S. nigrum and S. lycopersicum by high Cd stress, higher increase occurred in the tissues of S. lycopersicum. The concentration of free proline in the leaves and roots of S. nigrum was higher than those in S. lycopersicum across all the Cd treatments. These results showed that the Cdhyperaccumulator, S. nigrum had a greater capacity than S. lycopersicum to adapt to oxidative stress caused by Cd.Key words: Solanum nigrum L., hyperaccumulator, antioxidative defense, proline, cadmium

    Magnetization reversal through synchronization with a microwave

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    Based on the Landau-Lifshitz-Gilbert equation, it can be shown that a circularly-polarized microwave can reverse the magnetization of a Stoner particle through synchronization. In comparison with magnetization reversal induced by a static magnetic field, it can be shown that when a proper microwave frequency is used the minimal switching field is much smaller than that of precessional magnetization reversal. A microwave needs only to overcome the energy dissipation of a Stoner particle in order to reverse magnetization unlike the conventional method with a static magnetic field where the switching field must be of the order of magnetic anisotropy.Comment: 4 pages, 5 figure

    Zero-field magnetization reversal of two-body Stoner particles with dipolar interaction

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    Nanomagnetism has recently attracted explosive attention, in particular, because of the enormous potential applications in information industry, e.g. new harddisk technology, race-track memory[1], and logic devices[2]. Recent technological advances[3] allow for the fabrication of single-domain magnetic nanoparticles (Stoner particles), whose magnetization dynamics have been extensively studied, both experimentally and theoretically, involving magnetic fields[4-9] and/or by spin-polarized currents[10-20]. From an industrial point of view, important issues include lowering the critical switching field HcH_c, and achieving short reversal times. Here we predict a new technological perspective: HcH_c can be dramatically lowered (including Hc=0H_c=0) by appropriately engineering the dipole-dipole interaction (DDI) in a system of two synchronized Stoner particles. Here, in a modified Stoner-Wohlfarth (SW) limit, both of the above goals can be achieved. The experimental feasibility of realizing our proposal is illustrated on the example of cobalt nanoparticles.Comment: 5 pages, 4 figure

    Exploring spin-orbital models with dipolar fermions in zig-zag optical lattices

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    Ultra-cold dipolar spinor fermions in zig-zag type optical lattices can mimic spin-orbital models relevant in solid-state systems, as transition-metal oxides with partially filled d-levels, with the interesting advantage of reviving the quantum nature of orbital fluctuations. We discuss two different physical systems in which these models may be simulated, showing that the interplay between lattice geometry and spin-orbital quantum dynamics produces a wealth of novel quantum phases.Comment: 4 pages + supplementary materia
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