5,521 research outputs found

    Critical behavior of density of states near Fermi energy in low-dimensional disordered metals

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    We study the effect of electron-electron interaction on the one-particle density of states (\emph{DOS}) ρ(d)(ϵ,T)\rho^{(d)}(\epsilon,T) of low-dimensional disordered metals near Fermi energy within the framework of the finite temperature conventional impurity diagram technique. We consider only diffusive limit and by a geometric re-summation of the most singular first order self-energy corrections via the Dyson equation we obtain a non-divergent solution for the \emph{DOS} at low energies, while for higher energies the well-known Altshuler-Aronov corrections are recovered. At the Fermi level ρ(d)(ϵ,T=0)0\rho^{(d)}(\epsilon,T=0)\to 0, this indicates that interacting disordered two- and quasi-one-dimensional systems are in insulating state at zero temperature. The obtained results are in good agreement with recent tunneling experiments on two-dimensional GaAs/AlGaAs heterostructures and quasi-one-dimensional doped multiwall carbon nanotubes.Comment: 8 pages, 4 figure

    Renormalization of hole-hole interaction at decreasing Drude conductivity

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    The diffusion contribution of the hole-hole interaction to the conductivity is analyzed in gated GaAs/Inx_xGa1x_{1-x}As/GaAs heterostructures. We show that the change of the interaction correction to the conductivity with the decreasing Drude conductivity results both from the compensation of the singlet and triplet channels and from the arising prefactor αi<1\alpha_i<1 in the conventional expression for the interaction correction.Comment: 6 pages, 5 figure

    A model for the accidental catalysis of protein unfolding in vivo

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    Activated processes such as protein unfolding are highly sensitive to heterogeneity in the environment. We study a highly simplified model of a protein in a random heterogeneous environment, a model of the in vivo environment. It is found that if the heterogeneity is sufficiently large the total rate of the process is essentially a random variable; this may be the cause of the species-to-species variability in the rate of prion protein conversion found by Deleault et al. [Nature, 425 (2003) 717].Comment: 5 pages, 2 figure

    Hole-hole interaction in a strained Inx_xGa1x_{1-x}As two dimensional system

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    The interaction correction to the conductivity of 2D hole gas in strained GaAs/Inx_xGa1x_{1-x}As/GaAs quantum well structures was studied. It is shown that the Zeeman splitting, spin relaxation and ballistic contribution should be taking into account for reliable determination of the Fermi-liquid constant F0σF_0^\sigma. The proper consideration of these effects allows us to describe both th temperature and magnetic field dependences of the conductivity and find the value of F0σF_0^\sigma.Comment: 7 pages, 6 figure

    Diffusion and ballistic contributions of the interaction correction to the conductivity of a two-dimensional electron gas

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    The results of an experimental study of interaction quantum correction to the conductivity of two-dimensional electron gas in A3_3B5_5 semiconductor quantum well heterostructures are presented for a wide range of TτT\tau-parameter (Tτ0.030.8T\tau\simeq 0.03-0.8), where τ\tau is the transport relaxation time. A comprehensive analysis of the magnetic field and temperature dependences of the resistivity and the conductivity tensor components allows us to separate the ballistic and diffusion parts of the correction. It is shown that the ballistic part renormalizes in the main the electron mobility, whereas the diffusion part contributes to the diagonal and does not to the off-diagonal component of the conductivity tensor. We have experimentally found the values of the Fermi-liquid parameters describing the electron-electron contribution to the transport coefficients, which are found in a good agreement with the theoretical results.Comment: 11 pages, 11 figure

    Giant suppression of the Drude conductivity due to quantum interference in disordered two-dimensional systems

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    Temperature and magnetic field dependences of the conductivity in heavily doped, strongly disordered two-dimensional quantum well structures GaAs/Inx_xGa1x_{1-x}As/GaAs are investigated within wide conductivity and temperature ranges. Role of the interference in the electron transport is studied in the regimes when the phase breaking length LϕL_\phi crosses over the localization length ξlexp(πkFl/2)\xi\sim l\exp{(\pi k_Fl/2)} with lowering temperature, where kFk_F and ll are the Fermi quasimomentum and mean free path, respectively. It has been shown that all the experimental data can be understood within framework of simple model of the conductivity over delocalized states. This model differs from the conventional model of the weak localization developed for kFl1k_Fl\gg 1 and LϕξL_\phi\ll\xi by one point: the value of the quantum interference contribution to the conductivity is restricted not only by the phase breaking length LϕL_\phi but by the localization length ξ\xi as well. We show that just the quantity (τϕ)1=τϕ1+τξ1(\tau_\phi^\ast)^{-1}=\tau_\phi^{-1}+\tau_\xi^{-1} rather than τϕ1\tau_\phi^{-1}, where τϕT1\tau_\phi\propto T^{-1} is the dephasing time and τξτexp(πkFl)\tau_\xi\sim\tau\exp(\pi k_F l), is responsible for the temperature and magnetic field dependences of the conductivity over the wide range of temperature and disorder strength down to the conductivity of order 102e2/h10^{-2} e^2/h.Comment: 11 pages, 15 figure

    `Third' Quantization of Vacuum Einstein Gravity and Free Yang-Mills Theories

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    Based on the algebraico-categorical (:sheaf-theoretic and sheaf cohomological) conceptual and technical machinery of Abstract Differential Geometry, a new, genuinely background spacetime manifold independent, field quantization scenario for vacuum Einstein gravity and free Yang-Mills theories is introduced. The scheme is coined `third quantization' and, although it formally appears to follow a canonical route, it is fully covariant, because it is an expressly functorial `procedure'. Various current and future Quantum Gravity research issues are discussed under the light of 3rd-quantization. A postscript gives a brief account of this author's personal encounters with Rafael Sorkin and his work.Comment: 43 pages; latest version contributed to a fest-volume celebrating Rafael Sorkin's 60th birthday (Erratum: in earlier versions I had wrongly written that the Editor for this volume is Daniele Oriti, with CUP as publisher. I apologize for the mistake.

    Local Moment Formation in the Superconducting State of a Doped Mott Insulator

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    A microscopic theory is presented for the local moment formation near a non-magnetic impurity or a copper defect in high-T_c superconductors. We use a renormalized meanfield theory of the t-J model for a doped Mott insulator and study the fully self-consistent, spatially unrestricted solutions of the d-wave superconducting (SC) state in both the spin S=0 and S=1/2 sectors. We find a transition from the singlet d-wave SC state to a spin doublet SC state when the renormalized exchange coupling exceeds a doping dependent critical value. The induced S=1/2 moment is staggered and localized around the impurity. It arises from the binding of an S=1/2 nodal quasiparticle excitation to the impurity. The local density of states spectrum is calculated and connections to NMR and STM experiments are discussed.Comment: 4 pages, 3 figures, revised version, to be published in Phys. Rev. Let

    Localized to extended states transition for two interacting particles in a two-dimensional random potential

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    We show by a numerical procedure that a short-range interaction uu induces extended two-particle states in a two-dimensional random potential. Our procedure treats the interaction as a perturbation and solve Dyson's equation exactly in the subspace of doubly occupied sites. We consider long bars of several widths and extract the macroscopic localization and correlation lengths by an scaling analysis of the renormalized decay length of the bars. For u=1u=1, the critical disorder found is Wc=9.3±0.2W_{\rm c}=9.3\pm 0.2, and the critical exponent ν=2.4±0.5\nu=2.4\pm 0.5. For two non-interacting particles we do not find any transition and the localization length is roughly half the one-particle value, as expected.Comment: 4 two-column pages, 4 eps figures, Revtex, to be published in Europhys. Let
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