465 research outputs found

    Robustness of a local Fermi Liquid against Ferromagnetism and Phase Separation

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    We study the properties of Fermi Liquids with the microscopic constraint of a local self-energy. In this case the forward scattering sum-rule imposes strong limitations on the Fermi-Liquid parameters, which rule out any Pomeranchek instabilities. For both attractive and repulsive interactions, ferromagnetism and phase separation are suppressed. Superconductivity is possible in an s-wave channel only. We also study the approach to the metal-insulator transition, and find a Wilson ratio approaching 2. This ratio and other properties of Sr_{1-x}La_xTiO_3 are all consistent with the local Fermi Liquid scenario.Comment: 4 pages (twocolumn format), can compile with or without epsf.sty latex style file -- Postscript files: fig1.ps and fig2.p

    Low-Temperature Spin Diffusion in a Spin-Polarized Fermi Gas

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    We present a finite temperature calculation of the transverse spin-diffusion coefficient, DD_\bot, in a dilute degenerate Fermi gas in the presence of a small external magnetic field, HH. While the longitudinal diffusion coefficient displays the conventional low-temperature Fermi-liquid behavior, DT2D_\parallel \propto T^{-2}, the corresponding results for DD_\bot show three separate regimes: (a) DH2D_\bot \sim H^{-2} for THT \ll H; (b) DT2D_\bot \sim T^{-2}, D/D1D_\bot /D_\parallel \neq 1 for THT \gg H and large spin-rotation parameter ξ1\xi \gg 1, and (c) D=DT2D_\bot = D_\parallel \propto T^{-2} for THT \gg H and ξ1\xi \ll 1. Our results are qualitatively consistent with the available experimental data in weakly spin-polarized 3He^3{\rm He} and 3He4He^3{\rm He} - ^4{\rm He} mixtures.Comment: 13 pages, REVTEX, 3 figures available upon request, RU-94-4

    Dynamic Exponent of t-J and t-J-W Model

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    Drude weight of optical conductivity is calculated at zero temperature by exact diagonalization for the two-dimensional t-J model with the two-particle term, WW. For the ordinary t-J model with WW=0, the scaling of the Drude weight Dδ2D \propto \delta^2 for small doping concentration δ\delta is obtained, which indicates anomalous dynamic exponent zz=4 of the Mott transition. When WW is switched on, the dynamic exponent recovers its conventional value zz=2. This corresponds to an incoherent-to-coherent transition associated with the switching of the two-particle transfer.Comment: LaTeX, JPSJ-style, 4 pages, 5 eps files, to appear in J. Phys. Soc. Jpn. vol.67, No.6 (1998

    Quasiparticle dynamics and phonon softening in FeSe superconductors

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    Quasiparticle dynamics of FeSe single crystals revealed by dual-color transient reflectivity measurements ({\Delta}R/R) provides unprecedented information on Fe-based superconductors. The amplitude of fast component in {\Delta}R/R clearly tells a competing scenario between spin fluctuations and superconductivity. Together with the transport measurements, the relaxation time analysis further exhibits anomalous changes at 90 K and 230 K. The former manifests a structure phase transition as well as the associated phonon softening. The latter suggests a previously overlooked phase transition or crossover in FeSe. The electron-phonon coupling constant {\lambda} is found to be 0.16, identical to the value of theoretical calculations. Such a small {\lambda} demonstrates an unconventional origin of superconductivity in FeSe.Comment: Final published version; 5 pages; 4 figure

    Impact of interface traps on charge noise, mobility and percolation density in Ge/SiGe heterostructures

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    Hole spins in Ge/SiGe heterostructure quantum dots have emerged as promising qubits for quantum computation. The strong spin-orbit coupling (SOC), characteristic of heavy-hole states in Ge, enables fast and all-electrical qubit control. However, SOC also increases the susceptibility of spin qubits to charge noise. While qubit coherence can be significantly improved by operating at sweet spots with reduced hyperfine or charge noise sensitivity, the latter ultimately limits coherence, underlining the importance of understanding and reducing charge noise at its source. In this work, we study the voltage-induced hysteresis commonly observed in SiGe-based quantum devices and show that the dominant charge fluctuators are localized at the semiconductor-oxide interface. By applying increasingly negative gate voltages to Hall bar and quantum dot devices, we investigate how the hysteretic filling of interface traps impacts transport metrics and charge noise. We find that the gate-induced accumulation and trapping of charge at the SiGe-oxide interface leads to an increased electrostatic disorder, as probed by transport measurements, as well as the activation of low-frequency relaxation dynamics, resulting in slow drifts and increased charge noise levels. Our results highlight the importance of a conservative device tuning strategy and reveal the critical role of the semiconductor-oxide interface in SiGe heterostructures for spin qubit applications

    Direct Calculation of Spin-Stiffness for Spin-1/2 Heisenberg Models

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    The spin-stiffness of frustrated spin-1/2 Heisenberg models in one and two dimensions is computed for the first time by exact diagonalizations on small clusters that implement spin-dependent twisted boundary conditions. Finite-size extrapolation to the thermodynamic limit yields a value of 0.14±0.010.14\pm 0.01 for the spin-stiffness of the unfrustrated planar antiferromagnet. We also present a general discussion of the linear-response theory for spin-twists, which ultimately leads to the moment sum-rule.Comment: 11 pgs, TeX, LA-UR-94-94 (to be published in Phys. Rev. B

    Hidden spin-current conservation in 2d Fermi liquids

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    We report the existence of regimes of the two dimensional Fermi liquid that show unusual conservation of the spin current and may be tuned by varying some parameter like the density of fermions. We show that for reasonable models of the effective interaction the spin current may be conserved in general in 2d, not only for a particular regime. Low temperature spin waves propagate distinctively in these regimes and entirely new ``spin-acoustic'' modes are predicted for scattering-dominated temperature ranges. These new high-temperature propagating spin waves provide a clear signature for the experimental search of such regimes.Comment: 4 pages, no figures, revised version, accepted for pub. in the PR

    No Massive Companion to the Coherent Radio-Emitting M Dwarf GJ 1151

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    The recent detection of circularly polarized, long-duration (>8 hr) low-frequency (~150 MHz) radio emission from the M4.5 dwarf GJ 1151 has been interpreted as arising from a star-planet interaction via the electron cyclotron maser instability. The existence or parameters of the proposed planets have not been determined. Using 20 new HARPS-N observations, we put 99th-percentile upper limits on the mass of any close companion to GJ 1151 at Msini < 5.6 M earth. With no stellar, brown dwarf, or giant planet companion likely in a close orbit, our data are consistent with detected radio emission emerging from a magnetic interaction between a short-period terrestrial-mass planet and GJ 1151

    Nodes of the Gap Function and Anomalies in Thermodynamic Properties of Superfluid 3^3He

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    Departures of thermodynamic properties of three-dimensional superfluid 3^3He from the predictions of BCS theory are analyzed. Attention is focused on deviations of the ratios Δ(T=0)/Tc\Delta(T=0)/T_c and [Cs(Tc)Cn(Tc)]/Cn(Tc)[C_s(T_c)-C_n(T_c)]/C_n(T_c) from their BCS values, where Δ(T=0)\Delta(T=0) is the pairing gap at zero temperature, TcT_c is the critical temperature, and CsC_s and CnC_n are the superfluid and normal specific heats. We attribute these deviations to the momentum dependence of the gap function Δ(p)\Delta(p), which becomes well pronounced when this function has a pair of nodes lying on either side of the Fermi surface. We demonstrate that such a situation arises if the P-wave pairing interaction V(p1,p2)V(p_1,p_2), evaluated at the Fermi surface, has a sign opposite to that anticipated in BCS theory. Taking account of the momentum structure of the gap function, we derive a closed relation between the two ratios that contains no adjustable parameters and agrees with the experimental data. Some important features of the effective pairing interaction are inferred from the analysis.Comment: 17 pages, 4 figure
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