Nonstationary Stochastic ResonanceIt is by now established that, remarkably, the addition of noise to a nonlinear system may sometimes facilitate, rather than hamper the detection of weak signals. This phenomenon, usually referred to…Redouane Fakir·Mar 24, 1998SaveLearn
Nonstationary Stochastic Resonance in a Single Neuron-Like SystemStochastic resonance holds much promise for the detection of weak signals in the presence of relatively loud noise. Following the discovery of nondynamical and of aperiodic stochastic resonance, it…Redouane Fakir·Mar 23, 1998SaveLearn
A geometric generalization of field theory to manifolds of arbitrary dimensionWe introduce a generalization of the O(N) field theory to N-colored membranes of arbitrary inner dimension D. The O(N) model is obtained for D->1, while N->0 leads to self-avoiding tethered membranes…Kay Joerg Wiese, Mehran Kardar·Mar 23, 1998SaveLearn
Perturbation Theory for Singular Potentials in Quantum MechanicsWe study perturbation theory in certain quantum mechanics problems in which the perturbing potential diverges at some points, even though the energy eigenvalues are smooth functions of the…Diptiman Sen·Mar 23, 1998SaveLearn
Addendum to paper: Strong-Coupling Behavior of ϕ4-Theories and Critical Exponents [Phys. Rev. D 57, 2264 (1998)]The graphical extrapolation procedure to infinite order of variational perturbation theory in a recent calculation of critical exponents of three-dimensional ϕ4-theories at infinite couplings is…Hagen Kleinert·Mar 22, 1998SaveLearn
Universal Spin Response in Copper Oxide MaterialsThe spin response in the copper oxide materials at finite temperatures in the underdoped and optimal doped regimes is studied within the framework of the fermion-spin theory. The integrated dynamical…Shiping Feng, Zhongbing Huang·Mar 20, 1998SaveLearn
Transitions between Phases with Equal Wave Numbers in a Double Ising Spin Model. Application to Betaine Calcium Chloride DihydrateA Double Ising Spin model for uniaxially structurally modulated materials exhibits as a special feature phase transitions between phases with equal wave numbers but different pseudo spin…Boris Neubert, Michel Pleimling, Rolf Siems·Mar 20, 1998SaveLearn
Analysis of data sets of stochastic systemsThis paper deals with the analysis of stochastic systems which can be described by a Langevin equation. By the method presented in this paper drift and diffusion terms of the corresponding…S. Siegert, R. Friedrich, J. Peinke·Mar 20, 1998SaveLearn
Scaling Function for the Critical Specific Heat in a Confined Geometry : Spherical LimitThe scaling function for the critical specific heat is obtained exactly for temperatures above the bulk transition temperature by working in the spherical limit. Generalization of the function to…Saugata Bhattacharyya, J. K. Bhattacharjee·Mar 20, 1998SaveLearn
Critical Ultrasonics Near the Superfluid Transition : Finite Size EffectsThe suppression of order parameter fluctuations at the boundaries causes the ultrasonic attenuation near the superfluid transition to be lowered below the bulk value. We calculate explicitly the…Saugata Bhattacharyya, J. K. Bhattacharjee·Mar 20, 1998SaveLearn
Intensity distribution for waves in disordered media: deviations from Rayleigh statisticsWe study the intensity distribution function, P(I), for monochromatic waves propagating in quasi one-dimensional disordered medium, assuming that a point source and a point detector are embedded in…A. D. Mirlin, R. Pnini, B. Shapiro·Mar 20, 1998SaveLearn
Two-dimensional Coulomb systems on a surface of constant negative curvatureWe study the equilibrium statistical mechanics of classical two-dimensional Coulomb systems living on a pseudosphere (an infinite surface of constant negative curvature). The Coulomb potential…B. Jancovici, G. Tellez·Mar 20, 1998SaveLearn
Vortices and the Ginzburg-Landau phase transitionThe methods for studying the role of vortex loops in the phase transition of the Ginzburg-Landau theory of superconductivity using lattice Monte Carlo simulations are discussed. Gauge-invariant…A. Rajantie·Mar 18, 1998SaveLearn
Gauge invariant grid discretization of Schrödinger equationUsing the Wilson formulation of lattice gauge theories, a gauge invariant grid discretization of a one-particle Hamiltonian in the presence of an external electromagnetic field is proposed. This…M. Governale, C. Ungarelli·Mar 18, 1998SaveLearn
Spinor Bose Condensates in Optical TrapsIn an optical trap, the ground state of spin-1 Bosons such as 23Na, 39K, and 87Rb can be either a ferromagnetic or a "polar" state, depending on the scattering lengths in…Tin-Lun Ho·Mar 18, 1998SaveLearn
Elimination of unoccupied state summations in ab-initio self-energy calculations for large supercellsWe present a new method for the computation of self-energy corrections in large supercells. It eliminates the explicit summation over unoccupied states, and uses an iterative scheme based on an…Lucia Reining, Giovanni Onida, R. W. Godby·Mar 18, 1998SaveLearn
Analytical expressions for the local-field factor G(q) and the exchange-correlation kernel Kxc(r) of the homogeneous electron gasWe present an analytical expression for the local field factor G(q) of the homogeneous electron gas which reproduces recently published Quantum Monte--Carlo data by S. Moroni, D.M. Ceperley, and G.…Massimiliano Corradini, Rodolfo Del Sole, Giovanni Onida et al.·Mar 18, 1998SaveLearn
Dynamics of Dry Friction: A Numerical InvestigationWe perform extended numerical simulation of the dynamics of dry friction, based on a model derived from the phenomenological description proposed by T. Baumberger et al.. In the case of small…Y. F. Lim, Kan Chen·Mar 18, 1998SaveLearn
Analytical description of a trapped semi-ideal Bose gas at finite temperaturePresent experiments with Bose condensed gases can be largely described by a semi-ideal two-gas model. In this model, the condensate is influenced only by the mean-field repulsion among condensed…M. Naraschewski, D. M. Stamper-Kurn·Mar 18, 1998SaveLearn
Algebraic Bethe ansatz for the supersymmetric t-J model with reflecting boundary conditionsIn the framework of the graded quantum inverse scattering method (QISM), we obtain the eigenvalues and eigenvectors of the supersymmetric t-J model with reflecting boundary conditions in FFB…Heng Fan, Bo-yu Hou, Kang-jie Shi·Mar 18, 1998SaveLearn
Dispersion relations and speeds of sound in special sectors for the integrable chain with alternating spinsBased on our previous analysis doerfel3 of the anisotropic integrable chain consisting of spins s=1/2 and s=1 we compare the dispersion relations for the sectors with infinite Fermi zones.…B. -D. Doerfel, St. Meissner·Mar 17, 1998SaveLearn
Diffusion Quantum Monte Carlo Calculations of Excited States of SiliconThe band structure of silicon is calculated at the Gamma, X, and L wave vectors using diffusion quantum Monte Carlo methods. Excited states are formed by promoting an electron from the valence band…A. J. Williamson, Randolph Q. Hood, R. J. Needs et al.·Mar 17, 1998SaveLearn
Surface Screening Charge and Effective ChargeThe charge on an atom at a metallic surface in an electric field is defined as the field-derivative of the force on the atom, and this is consistent with definitions of effective charge and screening…S. Clarke, J. E. Inglesfield, M. Nekovee et al.·Mar 16, 1998SaveLearn
Jamming, Force Chains and Fragile MatterWe consider materials whose mechanical integrity is the result of a jamming process. We argue that such media are generically "fragile": unable to support certain types of incremental loading…M. E. Cates, J. Wittmer, J. P. Bouchaud et al.·Mar 16, 1998SaveLearn
Rod-like Polyelectrolytes in Presence of Monovalent SaltWe investigate the properties of rigid polyelectrolyte solutions in presence of monovalent salt. The free energy within the Debye-Hückel-Bjerrum (DHBj) theory [M. E. Fisher and Y. Levin, Phys.…Paulo S. Kuhn, Yan Levin, Marcia C. Barbosa·Mar 16, 1998SaveLearn