Current-Induced Chiral Phase Transition in a Josephson-Junction ArrayIt is predicted that the fully frustrated Josephson-junction array on a square lattice with alternating columns of junctions having a reduced critical current Iweak=μI0(with μ<1 and I0…M. V. Simkin·Apr 30, 1996SaveLearn
Impurity scattering and localization in d-wave superconductorsStrong evidence is presented for the localization of low energy quasiparticle states in disordered d-wave superconductors. Within the framework of the Bogoliubov-de Gennes (BdG) theory applied to…M. Franz, C. Kallin, A. J. Berlinsky·Apr 30, 1996SaveLearn
Long Wavelength Instability for Uniform Shear FlowUniform Shear Flow is a prototype nonequilibrium state admitting detailed study at both the macroscopic and microscopic levels via theory and computer simulation. It is shown that the hydrodynamic…Mirim Lee, James W. Dufty, José M. Montanero et al.·Apr 30, 1996SaveLearn
Nonlocal Conductivity in the Vortex-Liquid Regime of a Two-Dimensional SuperconductorWe have simulated the time-dependent Ginzburg-Landau equation with thermal fluctuations, to study the nonlocal dc conductivity of a superconducting film. Having examined points in the phase diagram…Rachel Wortis, David A. Huse·Apr 30, 1996SaveLearn
Resistance of superconductor-normal metal-superconductor junctionsIt is shown that the conductance of a superconductor-normal metal-superconductor junction can exhibit a significant dependence on the phase of the superconducting order parameter in the situation…F. Zhou, B. Spivak·Apr 30, 1996SaveLearn
Glassy Motion of Elastic ManifoldsWe discuss the low-temperature dynamics of an elastic manifold driven through a random medium. For driving forces well below the T=0 depinning force, the medium advances via thermally activated…Valerii M. Vinokur, M. Cristina Marchetti, Lee-Wen Chen·Apr 30, 1996SaveLearn
A Microscopic Derivation of the Critical Magnetic Field in a SuperconductorThe propagator for a noninteracting many electron system in a constant magnetic field in three space time dimensions is computed. This formula and the results of [FT1,2] are used to give a…Detlef Lehmann·Apr 30, 1996SaveLearn
Investigation of the Spin-Peierls transition in CuGeO3 by Raman scatteringRaman experiments on the spin-Peierls compound CuGeO3 and the substituted (Cu1- x,Znx)GeO3 and Cu(Ge1-x,Gax)O3 compounds were performed in order to investigate the response…P. Lemmens, B. Eisener, M. Brinkmann et al.·Apr 30, 1996SaveLearn
Computer simulation of crystallization kinetics with non-Poisson distributed nucleiThe influence of non-uniform distribution of nuclei on crystallization kinetics of amorphous materials is investigated. This case cannot be described by the well-known Johnson-Mehl-Avrami (JMA)…Patric Uebele, Helmut Hermann·Apr 30, 1996SaveLearn
Comment on "Voltage-Current Characteristics of the Two-Dimensional Gauge Glass Model"Li (Phys. Rev. Lett. 69,1819 (1992)) has computed the current-voltage characteristics (CVC) of a disordered two-dimensional (2D) Josephson-junction array and claimed that his data(nonlinear CVC…M. V. Simkin·Apr 30, 1996SaveLearn
Indications of a Metallic Antiferromagnetic Phase in the 2 Dimensional U-t-t' ModelWe present mean-field and quantum Monte Carlo results that suggest the existence of an itinerant antiferromagnetic ground state in the half-filled U-t-t' model in two dimensions. In particular,…Daniel Duffy, Adriana Moreo·Apr 29, 1996SaveLearn
Variational Monte Carlo and Configurational Interaction Studies of C60 and its FragmentsThe C60 molecule and its fragments are studied using Configuration Interaction (CI) and Variational Monte Carlo (VMC) techniques, within the Hubbard model. Using benzene as a test case, we…Bhargavi Srinivasan, S. Ramasesha, H. R. Krishnamurthy·Apr 29, 1996SaveLearn
Long-range effects on optical absorption in quasiperiodic latticesWe consider exciton optical absorption in quasiperiodic lattices, focusing our attention on the Fibonacci case as typical example. The absorption spectrum is evaluated by solving numerically the…Francisco Dominguez-Adame·Apr 29, 1996SaveLearn
Nonzero Fermi Level Density of States for a Disordered d-Wave SuperconductorIt has been known for some time that, in three dimensions, arbitrarily weak disorder in unconventional superconductors with line nodes gives rise to a nonzero residual density of zero-energy…Klaus Ziegler, Matthias H. Hettler, Peter J. Hirschfeld·Apr 29, 1996SaveLearn
Multi-configurational Symmetrized Projector Quantum Monte Carlo Studies of excited states of the Hubbard modelWe develop a novel multi-configurational Symmetrized Projector Quantum Monte Carlo (MSPQMC) method to calculate excited state properties of Hubbard models. We compare the MSPQMC results for finite…Bhargavi Srinivasan, S. Ramasesha, H. R. Krishnamurthy·Apr 29, 1996SaveLearn
Dissipative Chaos in Semiconductor SuperlatticesWe consider the motion of ballistic electrons in a miniband of a semiconductor superlattice (SSL) under the influence of an external, time-periodic electric field. We use the semi-classical…Kirill N. Alekseev, Gennady P. Berman, David K. Campbell et al.·Apr 29, 1996SaveLearn
Field-driven topological glass transition in a model flux line latticeWe show that the flux line lattice in a model layered HTSC becomes unstable above a critical magnetic field with respect to a plastic deformation via penetration of pairs of point-like disclination…Seungoh Ryu, A. Kapitulnik, S. Doniach·Apr 29, 1996SaveLearn
Unconventional Ferromagnetic Transition in La1-xCaxMnO3Neutron scattering has been used to study the magnetic correlations and long wavelength spin dynamics of La1-xCaxMnO3 in the ferromagnetic regime (0<=x<1/2). For x=1/3 (Tc=250K) where the…J. W. Lynn, R. W. Erwin, J. A. Borchers et al.·Apr 29, 1996SaveLearn
Percolation and cluster Monte Carlo dynamics for spin modelsA general scheme for devising efficient cluster dynamics proposed in a previous letter [Phys.Rev.Lett. 72, 1541 (1994)] is extensively discussed. In particular the strong connection among equilibrium…V. Cataudella, G. Franzese, M. Nicodemi et al.·Apr 29, 1996SaveLearn
Kondo lattice model: Unitary transformations, spin dynamics, strongly correlated charged modes, and vacuum instabilityUsing unitary transformations, we express the Kondo lattice Hamiltonian in terms of fermionic operators that annihilate the ground state of the interacting system and that represent the best possible…J. M. Prats, F. Lopez-Aguilar·Apr 29, 1996SaveLearn
Critical dimensions for random walks on random-walk chainsThe probability distribution of random walks on linear structures generated by random walks in d-dimensional space, Pd(r,t), is analytically studied for the case ξ r/t1/41. It is…Savely Rabinovich, H. Eduardo Roman, Shlomo Havlin et al.·Apr 29, 1996SaveLearn
Scaling above the upper critical dimension in Ising ModelsWe rederive the finite size scaling formula for the apparent critical temperature by using Mean Field Theory for the Ising Model above the upper critical dimension. We have also performed numerical…Giorgio Parisi, Juan J. Ruiz-Lorenzo·Apr 29, 1996SaveLearn
Conductance Increase by Electron-Phonon Interaction in Quantum WiresWe investigate the influence of electron-phonon interactions on the DC-conductance Γ of a quantum wire in the limit of one occupied subband. At zero temperature, a Tomonaga-Luttinger-like…Tobias Brandes, Arisato Kawabata·Apr 28, 1996SaveLearn
Magnetoresistance of Two-Dimensional Fermions in a Random Magnetic FieldWe perform a semiclassical calculation of the magnetoresistance of spinless two-dimensional fermions in a long-range correlated random magnetic field. In the regime relevant for the problem of the…D. V. Khveshchenko·Apr 27, 1996SaveLearn
Surface Waves and Forced Oscillations in QHE Planar SamplesDispersion relations and polarizations for surface waves in infinite planar samples in the QHE regime are explicitly determined in the small wavevector limit in which the dielectric tensor can be…A. Cabo, A. Correa, R. Guevara et al.·Apr 26, 1996SaveLearn