116 research outputs found

    Optically-Induced Polarons in Bose-Einstein Condensates: Monitoring Composite Quasiparticle Decay

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    Nonresonant light-scattering off atomic Bose-Einstein condensates (BECs) is predicted to give rise to hitherto unexplored composite quasiparticles: unstable polarons, i.e., local ``impurities'' dressed by virtual phonons. Optical monitoring of their spontaneous decay can display either Zeno or anti-Zeno deviations from the Golden Rule, and thereby probe the temporal correlations of elementary excitations in BECs.Comment: 4 pages, 3 figure

    Metal-Insulator Transition and Spin Degree of Freedom in Silicon 2D Electron Systems

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    Magnetotransport in 2DES's formed in Si-MOSFET's and Si/SiGe quantum wells at low temperatures is reported. Metallic temperature dependence of resistivity is observed for the n-Si/SiGe sample even in a parallel magnetic field of 9T, where the spins of electrons are expected to be polarized completely. Correlation between the spin polarization and minima in the diagonal resistivity observed by rotating the samples for various total strength of the magnetic field is also investigated.Comment: 3 pages, RevTeX, 4 eps-figures, conference paper (EP2DS-13

    Cyclotron effective mass of 2D electron layer at GaAs/AlGaAs heterojunction subject to in-plane magnetic fields

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    We have found that Fermi contours of a two-dimensional electron gas at \rmGaAs/Al_xGa_{1-x}As interface deviate from a standard circular shape under the combined influence of an approximately triangular confining potential and the strong in-plane magnetic field. The distortion of a Fermi contour manifests itself through an increase of the electron effective cyclotron mass which has been measured by the cyclotron resonance in the far-infrared transmission spectra and by the thermal damping of Shubnikov-de Haas oscillations in tilted magnetic fields with an in-plane component up to 5 T. The observed increase of the cyclotron effective mass reaches almost 5 \% of its zero field value which is in good agreement with results of a self-consistent calculation.Comment: 4 pages, Revtex, figures can be obtained on request from [email protected]; to appear in Phys. Rev. B (in press). No changes, the corrupted submission replace

    A Droplet State in an Interacting Two-Dimensional Electron System

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    It is well known that the dielectric constant of two-dimensional (2D) electron system goes negative at low electron densities. A consequence of the negative dielectric constant could be the formation of the droplet state. The droplet state is a two-phase coexistence region of high density liquid and low density "gas". In this paper, we carry out energetic calculations to study the stability of the droplet ground state. The possible relevance of the droplet state to recently observed 2D metal-insulator transition is also discussed.Comment: 4 pages, 4 figures. To appear in Phys. Rev. B (Rapid Communications

    Fractional Systems and Fractional Bogoliubov Hierarchy Equations

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    We consider the fractional generalizations of the phase volume, volume element and Poisson brackets. These generalizations lead us to the fractional analog of the phase space. We consider systems on this fractional phase space and fractional analogs of the Hamilton equations. The fractional generalization of the average value is suggested. The fractional analogs of the Bogoliubov hierarchy equations are derived from the fractional Liouville equation. We define the fractional reduced distribution functions. The fractional analog of the Vlasov equation and the Debye radius are considered.Comment: 12 page

    Remarks on Shannon's Statistical Inference and the Second Law in Quantum Statistical Mechanics

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    We comment on a formulation of quantum statistical mechanics, which incorporates the statistical inference of Shannon. Our basic idea is to distinguish the dynamical entropy of von Neumann, H=kTrρ^lnρ^H = -k Tr \hat{\rho}\ln\hat{\rho}, in terms of the density matrix ρ^(t)\hat{\rho}(t), and the statistical amount of uncertainty of Shannon, S=knpnlnpnS= -k \sum_{n}p_{n}\ln p_{n}, with pn=p_{n}= in the representation where the total energy and particle numbers are diagonal. These quantities satisfy the inequality SHS\geq H. We propose to interprete Shannon's statistical inference as specifying the {\em initial conditions} of the system in terms of pnp_{n}. A definition of macroscopic observables which are characterized by intrinsic time scales is given, and a quantum mechanical condition on the system, which ensures equilibrium, is discussed on the basis of time averaging. An interesting analogy of the change of entroy with the running coupling in renormalization group is noted. A salient feature of our approach is that the distinction between statistical aspects and dynamical aspects of quantum statistical mechanics is very transparent.Comment: 16 pages. Minor refinement in the statements in the previous version. This version has been published in Journal of Phys. Soc. Jpn. 71 (2002) 6

    Critical Dynamics of a Vortex Loop Model for the Superconducting Transition

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    We calculate analytically the dynamic critical exponent zMCz_{MC} measured in Monte Carlo simulations for a vortex loop model of the superconducting transition, and account for the simulation results. In the weak screening limit, where magnetic fluctuations are neglected, the dynamic exponent is found to be zMC=3/2z_{MC} = 3/2. In the perfect screening limit, zMC=5/2z_{MC} = 5/2. We relate zMCz_{MC} to the actual value of zz observable in experiments and find that z2z \sim 2, consistent with some experimental results

    Quasiparticle Effective Mass for the Two- and Three-Dimensional Electron Gas

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    We calculate the quasiparticle effective mass for the electron gas in two and three dimensions in the metallic region. We employ the single particle scattering potential coming from the Sj\"{o}lander-Stott theory and enforce the Friedel sum rule by adjusting the effective electron mass in a scattering calculation. In 3D our effective mass is a monotonically decreasing function of rsr_s throughout the whole metallic domain, as implied by the most recent numerical results. In 2D we obtain reasonable agreement with the experimental data, as well as with other calculations based on the Fermi liquid theory. We also present results of a variety of different treatments for the effective mass in 2D and 3D.Comment: 12 pages, 2 figure

    Correlation energy and spin polarization in the 2D electron gas

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    The ground state energy of the two--dimensional uniform electron gas has been calculated with fixed--node diffusion Monte Carlo, including backflow correlations, for a wide range of electron densities as a function of spin polarization. We give a simple analytic representation of the correlation energy which fits the density and polarization dependence of the simulation data and includes several known high- and low-density limits. This parametrization provides a reliable local spin density energy functional for two-dimensional systems and an estimate for the spin susceptibility. Within the proposed model for the correlation energy, a weakly first--order polarization transition occurs shortly before Wigner crystallization as the density is lowered.Comment: Minor typos corrected, see erratum: Phys. Rev. Lett. 91, 109902(E) (2003

    Two - Dimensional Electron Liquid in a Weak Magnetic Field

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    We present an effective theory describing the low-energy properties of an interacting 2D electron gas at large non-integer filling factors ν1\nu\gg 1. Assuming that the interaction is sufficiently weak, rs<1r_s < 1, we integrate out all the fast degrees of freedom, and derive the effective Hamiltonian acting in the Fock space of the partially filled Landau level only. This theory enables us to find two energy scales controlling the electron dynamics at energies less than ωc\hbar\omega_c. The first energy scale, (ωc/ν)ln(νrs)(\hbar\omega_c/\nu)\ln\left(\nu r_s\right), appears in the one electron spectral density as the width of a pseudogap. The second scale, rsωcr_s\hbar\omega_c, is parametrically larger; it characterizes the exchange-enhanced spin splitting and the thermodynamic density of states.Comment: Submitted in Phys. Rev. B, 30 pages, 3 figures upon reques
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