Spin wave mediated non-reciprocal effects in antiferromagnetsBy using an effective field theory for the electromagnetic interaction of spin waves, we show that, in certain antiferromagnets, the latter induce non-reciprocal effects in the microwave region,…J. M. Roman, J. Soto·Sep 26, 1997SaveLearn
Effective Field Theory Approach to Ferromagnets and Antiferromagnets in Crystaline SolidsWe present a systematic construction of effective lagrangians for the low energy and momentum region of ferromagnetic and antiferromagnetic spin waves in crystalline solids. We fully exploit the…J. M. Roman, J. Soto·Sep 26, 1997SaveLearn
Spin holography IIThe interference of the directly emitted photoelectron wave and the wave scattered coherently by neighboring atoms gives holographic fringes in the photoelectron emission intensity I( R).…Eddy Timmermans, G. T. Trammell, J. P. Hannon·Sep 26, 1997SaveLearn
Theoretical analysis of the experiments on the double-spin-chain compound -- KCuCl3We have analyzed the experimental susceptibility data of KCuCl3 and found that the data are well-explained by the double-spin-chain models with strong antiferromagnetic dimerization. Large quantum…Tota Nakamura, Kiyomi Okamoto·Sep 26, 1997SaveLearn
Dynamical fluctuations in an exactly solvable model of spin glassesIn this work we calculate the dynamical fluctuations at O(1/N) in the low temperature phase of the p=2 spherical spin glass model. We study the large-times asymptotic regimes and we find, in a…Matteo Campellone, Giorgio Parisi, Paola Ranieri·Sep 25, 1997SaveLearn
A Unified Construction of Variational Methods for the Nonlinear Schroedinger EquationBased on an approach introduced byGerjuoy, Rau, and Spruch, we constract variational principles in a systematic way for the nonlinear Schroedinger equation and obtain new variational principles for…Yeong E. Kim, Alexander L. Zubarev·Sep 24, 1997SaveLearn
From Tomonaga-Luttinger to Fermi liquid in transport through a tunneling barrierFinite length of a one channel wire results in crossover from a Tomonaga-Luttinger to Fermi liquid behavior with lowering energy scale. In condition that voltage drop (V) mostly occurs across a…Vadim Ponomarenko, Naoto Nagaosa·Sep 24, 1997SaveLearn
Redistribution of the Hole Spectral Weight due to Long-Range Spin Correlations in the Three-Band Hubbard ModelIn the framework of the three-band model for CuO2 plane in high-temperature superconductors the spectrum of the spin-polaron hole exitation is investigated. The problem is treated taking into…A. F. Barabanov, O. V. Urazaev, E. Zasinas et al.·Sep 24, 1997SaveLearn
Damping in dilute Bose gases: a mean-field approachDamping in a dilute Bose gas is investigated using a mean-field approximation which describes the coupled oscillations of condensate and non-condensate atoms in the collisionless regime. Explicit…S. Giorgini·Sep 24, 1997SaveLearn
Non-perturbative Results on Universal Quantities of Statistical Mechanics ModelsExact calculations of some universal quantities of two-dimensional statistical models in the vicinity of their fixed points are illustrated.G. Mussardo·Sep 23, 1997SaveLearn
Intrinsic Decoherence in Mesoscopic SystemsWe point out that even at the absolute zero of temperature environmental decoherence limits the destructive interference between time-reversed paths for an electron in a disordered metal, and thus…Maxim Vavilov, Vinay Ambegaokar·Sep 22, 1997SaveLearn
The Longuet-Higgins Phase and Charge Transport in Molecular RingsThe Longuet-Higgins-Berry's phase has remarkable consequences for charge transport in molecular rings. For generic (conical) crossing, where the phase is π, a vanishing cause can lead to a…J. E. Avron, J. Berger·Sep 22, 1997SaveLearn
Quasiparticle Lifetimes and the Conductivity Scattering RateWe compute the single-particle inverse lifetime, along with the conductivity-derived scattering rate, for a metallic system in an s-wave superconducting state. When both electron-phonon and…F. Marsiglio, J. P. Carbotte·Sep 22, 1997SaveLearn
Zero-temperature dynamic transition in the random field Ising model: A Monte Carlo studyThe dynamics of a random (quenched) field Ising model (in two dimension) at zero temperature in the presence of an additional sinusoidally oscillating homogeneous (in space) magnetic field has been…Muktish Acharyya·Sep 19, 1997SaveLearn
Dilute Bose gas in a torus: vortices and persistent currentsWe consider the excitation spectrum and stability of quantized vortices in a weakly-interacting Bose gas trapped in a toroidal container, and discuss the driven rotation of such a condensate.D. S. Rokhsar·Sep 18, 1997SaveLearn
Magneto-Roton Modes in the Ultra Quantum Crystal: Life and Death at Large Magnetic FieldThe Ultra Quantum Crystal (UQC) phases observed in quasi-one-dimensional conductors of the Bechgaard salts family under magnetic field exhibit both Spin Density Wave order and a Quantized Hall…Pascal Lederer, C. M. Chaves·Sep 18, 1997SaveLearn
Magnetoresistance of the double-tunnel-junction Coulomb Blockade with magnetic metalsWe have studied the Junction Magnetoresistance (JMR) and the Differential junction magnetoresistance (DJMR) for double tunnel junctions with magnetic metals in the Coulomb Blockade regime. Spikes are…Kingshuk Majumdar, Selman Hershfield·Sep 18, 1997SaveLearn
Structural Consequences of the Range of the Interatomic Potential: a Menagerie of ClustersWe have attempted to find the global minima of clusters containing between 20 and 80 atoms bound by the Morse potential as a function of the range of the interatomic force. The effect of decreasing…Jonathan Doye, David Wales·Sep 18, 1997SaveLearn
Theory of Spontaneous Polarization of Endohedral FullerenesA pseudo-Jahn-Teller model describing central atom distortions is proposed for endohedral fullerenes of the form A@C60 where A is either a rare gas or a metal atom. A critical (dimensionless)…Dennis P. Clougherty, Frederick G. Anderson·Sep 16, 1997SaveLearn
Polaron Dissociation at the Insulator-to-Metal TransitionConsidering the long range Coulomb interactions between large polarons in dielectrics, we propose a model for their crystallization when no bipolarons are formed. As the density increases, the…P. Quemerais, S. Fratini·Sep 16, 1997SaveLearn
Anomalous finite size spectrum in the S=1/2 two dimensional Heisenberg modelWe study the low energy spectrum of the nearest neighbor Heisenberg model on a square lattice as a function of the total spin S. By quantum Monte Carlo simulation we compute this spectrum for the…C. Lavalle, S. Sorella, A. Parola·Sep 16, 1997SaveLearn
Dynamical properties of the compounds CuGeO3 and α'--NaV2O5 at temperatures T≠ 0The dynamical structure factor of the frustrated spin 1/2 Heisenberg model for a series of frustration parameters at finite temperatures is presented. A sharp upper boundary of the spinon continuum…K. Fabricius, U. Löw·Sep 15, 1997SaveLearn
Fractal properties of clusters of colloidal magnetic particlesWe have studied the properties of clusters of colloidal magnetic particles generated from a 2D aggregation model with dipolar interparticle interactions. Particles diffuse off-lattice, experiencing…R. Pastor-Satorras, J. M. Rubi·Sep 15, 1997SaveLearn
The Phase Structure of Antiferromagnetic Ising Model in the Presence of FrustrationsThe antiferromagnetic Ising model in a magnetic field is considered on the Husimi tree. Using iteration technique we draw the plots of magnetization versus external field for different temperatures…A. Z. Akheyan, N. S. Ananikian, S. K. Dallakian·Sep 15, 1997SaveLearn
Spin-density Wave in Ising-coupled Antiferromagnetic ChainsThe effect of anisotropy in the nearest-neighbor spin interactions that couple N≥ 2 consecutive spin-1/2 antiferromagnetic chains is studied theoretically by considering the limit where the…J. P. Rodriguez, P. D. Sacramento, V. R. Vieira·Sep 13, 1997SaveLearn