Macroscopic Quantum Tunneling of a Fluxon in a Long Josephson JunctionMacroscopic quantum tunneling (MQT) for a single fluxon moving along a long Josephson junction is studied theoretically. To introduce a fluxon-pinning force, we consider inhomogeneities made by…Takeo Kato, Masatoshi Imada·Apr 26, 1996SaveLearn
Transition from localized to extended eigenstates in the ensemble of power-law random banded matricesWe study statistical properties of the ensemble of large N× N random matrices whose entries Hij decrease in a power-law fashion Hij|i-j|-α. Mapping the problem onto a…Alexander D. Mirlin, Yan V. Fyodorov, Frank-Michael Dittes et al.·Apr 26, 1996SaveLearn
Relaxation of frustration and gap enhancement by the lattice distortion in the Δ chainWe clarify an instability of the ground state of the Δ chain against the lattice distortion that increases a strength (λ) of a bond in each triangle. It relaxes the frustration and causes a…Tota Nakamura, Satoshi Takada·Apr 26, 1996SaveLearn
Coherent patterns and self-induced diffraction of electrons on a thin nonlinear layerElectron scattering on a thin layer where the potential depends self-consistently on the wave function has been studied. When the amplitude of the incident wave exceeds a certain threshold, a…O. M. Bulashenko, V. A. Kochelap, L. L. Bonilla·Apr 25, 1996SaveLearn
SO(3) nonlinear σ model for a doped quantum helimagnetA field theory describing the low-energy, long-wavelength sector of an incommensurate, spiral magnetic phase is derived from a spin-fermion model that is commonly used as a microscopic model for…Susanne Klee, Alejandro Muramatsu·Apr 25, 1996SaveLearn
The Ising-Kondo lattice with transverse field: an f-moment Hamiltonian for URu2Si2?We study the phase diagram of the Ising-Kondo lattice with transverse magnetic field as a possible model for the weak-moment heavy-fermion compound URu2Si2, in terms of two low-lying f singlets in…A. E. Sikkema, W. J. L. Buyers, I. Affleck et al.·Apr 25, 1996SaveLearn
Survival Probability of a Gaussian Non-Markovian Process: Application to the T=0 Dynamics of the Ising ModelWe study the decay of the probability for a non-Markovian stationary Gaussian walker not to cross the origin up to time t. This result is then used to evaluate the fraction of spins that do not…Satya N. Majumdar, Clément Sire·Apr 24, 1996SaveLearn
A Numerical Renormalization Group Study of a Kondo Hole in a One Dimensional Kondo InsulatorWe have studied a Kondo hole in a one-dimensional Kondo insulator at half-filling using a density matrix formulation of the numerical renormalization group. The Kondo hole introduces midgap states.…Clare C. Yu·Apr 24, 1996SaveLearn
Electrons, pseudoparticles, and quasiparticles in the one-dimensional many-electron problemWe generalize the concept of quasiparticle for one-dimensional (1D) interacting electronic systems. The and quasiparticles recombine the pseudoparticle colors c and s…J. M. P. Carmelo, A. H. Castro Neto·Apr 24, 1996SaveLearn
Topological ground-state excitations and symmetry in the many-electron one-dimensional problemWe consider the Hubbard chain in a magnetic field and chemical potential. We introduce a pseudohole basis where all states are generated from a single reference vacuum. This allows the evaluation for…J. M. P. Carmelo, N. M. R. Peres·Apr 24, 1996SaveLearn
Magneto-optical evidence of the percolation nature of the metal-insulator transition in the 2D electron systemWe compare the results of the transport and time-resolved magneto-luminescence measurements in disordered 2D electron systems in GaAs-AlGaAs heterostructures in the extreme quantum limit, in…I. V. Kukushkin, Vladimir I. Fal'ko, R. J. Haug et al.·Apr 24, 1996SaveLearn
Critical Behavior of the Flux-line Tension in Extreme Type-II SuperconductorsThe entropic corrections to the flux-line energy of extreme type-II superconductors are computed using a schematic dual Villain model description of the flux quanta. We find that the temperature…J. P. Rodriguez·Apr 24, 1996SaveLearn
Monte Carlo study of the growth of L12 ordered domains in fcc A3B binary alloysA Monte Carlo study of the late time growth of L12 ordered domains on a fcc A3B binary alloy is presented. The energy of the alloy has been modeled by a nearest neighbor interaction Ising…Carlos Frontera, Eduard Vives, Teresa Castán et al.·Apr 24, 1996SaveLearn
Long-range correlations in the wave functions of chaotic systemsWe study correlations of the amplitudes of wave functions of a chaotic system at large distances. For this purpose, a joint distribution function of the amplitudes at two distant points in a sample…Vladimir I. Fal'ko, K. B. Efetov·Apr 24, 1996SaveLearn
Critical Dynamics of the Contact Process with Quenched DisorderWe study critical spreading dynamics in the two-dimensional contact process (CP) with quenched disorder in the form of random dilution. In the pure model, spreading from a single particle at the…Adriana G. Moreira, Ronald Dickman·Apr 24, 1996SaveLearn
Dynamics of coupled quantum spin chainsStatic and dynamical properties of weakly coupled antiferromagnetic spin chains are treated using a mean--field approximation for the interchain coupling and exact results for the resulting effective…H. J. Schulz·Apr 23, 1996SaveLearn
Is Heteropolymer Freezing Well Described by the Random Energy Model?It is widely held that the Random Energy Model (REM) describes the freezing transition of a variety of types of heteropolymers. We demonstrate that the hallmark property of REM, statistical…Vijay S. Pande, Alexander Yu. Grosberg, Chris Joerg et al.·Apr 23, 1996SaveLearn
Dephasing time of composite fermionsWe study the dephasing of fermions interacting with a fluctuating transverse gauge field. The divergence of the imaginary part of the fermion self energy at finite temperatures is shown to result…Patrick A. Lee, Eduardo R. Mucciolo, Henrik Smith·Apr 23, 1996SaveLearn
Two-dimensional S=1/2 antiferromagnet on a plaquette latticeWe consider a simplified model of the magnetic structure of the two-dimensional compound CaV4O9 in terms of interacting square plaquettes of spins with two distinct antiferromagnetic exchange…S. V. Meshkov, D. Foerster·Apr 23, 1996SaveLearn
Exact solution and spectral flow for twisted Haldane-Shastry modelThe exact solution of the spin chain model with 1/r2 exchange is found for twisted boundary conditions. The spectrum thus obtained can be reproduced by the asymptotic Bethe ansatz. The spectral…T. Fukui, N. Kawakami·Apr 23, 1996SaveLearn
Correlations of Eigenfunctions in Disordered SystemsCorrelations of eigenfunctions, |ψk(r1)|2|ψl(r2)|2, in a disordered system are investigated. We derive general formulae expressing these correlation functions in terms of the…Ya. M. Blanter, A. D. Mirlin·Apr 22, 1996SaveLearn
Spin-Peierls states of quantum antiferromagnets on the Ca V4 O9 latticeWe discuss the quantum paramagnetic phases of Heisenberg antiferromagnets on the 1/5-depleted square lattice found in Ca V4 O9. The possible phases of the quantum dimer model on this lattice are…Subir Sachdev, N. Read·Apr 22, 1996SaveLearn
Coherent State path-integral simulation of many particle systemsThe coherent state path integral formulation of certain many particle systems allows for their non perturbative study by the techniques of lattice field theory. In this paper we exploit this strategy…M. Beccaria, B. Alles, F. Farchioni·Apr 22, 1996SaveLearn
Fractal formation and ordering in random sequential adsorptionWe reveal the fractal nature of patterns arising in random sequential adsorption of particles with continuum power-law size distribution, P(R) Rα-1, R R max. We find that the…N. V. Brilliantov, Yu. A. Andrienko, P. L. Krapivsky et al.·Apr 22, 1996SaveLearn
Can fractal-like spectra be experimentally observed in aperiodic superlattices?We numerically investigate the effects of inhomogeneities in the energy spectrum of aperiodic semiconductor superlattices, focusing our attention on Thue-Morse and Fibonacci sequences. In the absence…Enrique Macia, Francisco Dominguez-Adame·Apr 22, 1996SaveLearn