`Baryonic' bound-state instability in trapped fermionic atomsWe consider a homogeneous gas of spin-S fermionic atoms, as might occur near the center of an optical trap. In the case where all scattering lengths are negative and of the same magnitude we…A. S. Stepanenko, J. M. F. Gunn·Jan 27, 1999SaveLearn
Patterns arising from the interaction between scalar and vectorial instabilities in two-photon resonant Kerr cavitiesWe study pattern formation associated with the polarization degree of freedom of the electric field amplitude in a mean field model describing a nonlinear Kerr medium close to a two-photon resonance,…Miguel Hoyuelos, Daniel Walgraef, Pere Colet et al.·Jan 27, 1999SaveLearn
Reaction Diffusion Models in One Dimension with DisorderWe study a large class of 1D reaction diffusion models with quenched disorder using a real space renormalization group method (RSRG) which yields exact results at large time. Particles (e.g. of…Pierre Le Doussal, Cecile Monthus·Jan 27, 1999SaveLearn
Pseudogaps and Extrinsic Losses in Photoemission Experiments on Poorly Conducting SolidsIt is shown that a photoelectron, on being emitted from a conducting solid, suffers a substantial energy change due to ohmic losses. Almost all of this energy loss takes place after the electron…Robert Joynt·Jan 26, 1999SaveLearn
Group-Theoretical Analysis of Second Harmonic Generation at (110) and (111) Surfaces of AntiferromagnetsExtending our previous work we classify the nonlinear magneto-optical response at low index surfaces of fcc antiferromagnets, such as NiO. Antiferromagnetic bilayers are discussed here as models for…M. Trzeciecki, W. Hübner·Jan 26, 1999SaveLearn
Convective and Absolute Instabilities in the Subcritical Ginzburg-Landau EquationWe study the nature of the instability of the homogeneous steady states of the subcritical Ginzburg-Landau equation in the presence of group velocity. The shift of the absolute instability threshold…Pere Colet, Daniel Walgraef, Maxi San Miguel·Jan 26, 1999SaveLearn
AC-Conductivity of Pinned Charge Density Wave Fluctuations in Quasi One-Dimensional ConductorsQuasi one-dimensional conductors which undergo a Peierls transition to a charge density wave state at a temperature TP show a region of one-dimensional fluctuations above TP. The…W. Wonneberger·Jan 26, 1999SaveLearn
The Josephson Plasma Resonance in Bi2Sr2CaCu2O8 in a Tilted FieldThe dependence of the Josephson plasma frequency omegap in Bi2Sr2CaCu2O8 on a tilted field H is reported. Measurements over a large range of B and tilt angle theta allow a detailed comparison…Sibel P. Bayrakci, Ophelia K. C. Tsui, N. P. Ong et al.·Jan 26, 1999SaveLearn
Segregation of Granular Mixtures in a Rotating DrumWe formulate a phenomenological model for the segregation of binary mixtures of rough and smooth granular materials in a rotating drum. Our model successfully replicates a range of experimental…Sanjay Puri, Hisao Hayakawa·Jan 25, 1999SaveLearn
Generalized Lotka-Volterra (GLV) Models and Generic Emergence of Scaling Laws in Stock MarketsThis is a pedagogical review of the the Generalized Lotka-Volterra (GLV) model: wi(t+1) = lambda * wi(t) + a * W (t) - c * W (t) * wi(t) where i=1, >......, N and W= (w1 + w2 + ...wN)/N is the…Sorin Solomon·Jan 23, 1999SaveLearn
Modelling Molecular Motors as Folding-Unfolding CyclesWe propose a model for motor proteins based on a hierarchical Hamiltonian that we have previously introduced to describe protein folding. The proposed motor model has high efficiency and is…Alex Hansen, Mogens H. Jensen, Kim Sneppen et al.·Jan 22, 1999SaveLearn
Moment scaling at the sol - gel transitionTwo standard models of sol-gel transition are revisited here from the point of view of their fluctutations in various moments of both the mass-distribution and the gel-mass. Bond-percolation model is…R. Botet, M. Ploszajczak·Jan 22, 1999SaveLearn
Moment of inertia of a trapped superfluid gas of atomic FermionsThe moment of inertia of a trapped superfluid gas of atomic Fermions (6Li) is calculated as a function of two system parameters: temperature and deformation of the trap. For moderate deformations at…M. Farine, P. Schuck, X. Vinas·Jan 22, 1999SaveLearn
Influence of finite Hund rules and charge transfer on properties of Haldane systemsWe consider the Kondo-Hubbard model with ferromagnetic exchange coupling % JH, showing that it is an approximate effective model for late transition metal-O linear systems. We study the…A. E. Feiguin, Liliana Arrachea, A. A. Aligia·Jan 21, 1999SaveLearn
Algorithm for normal random numbersWe propose a simple algorithm for generating normally distributed pseudo random numbers. The algorithm simulates N molecules that exchange energy among themselves following a simple stochastic rule.…J. F. Fernandez, Carlos Criado·Jan 20, 1999SaveLearn
Stability and diffusion of surface clustersUsing kinetic Monte Carlo simulations and a bond-counting ansatz, thermal stability and diffusion of an adatom island on a crystal surface are studied. At low temperatures, the diffusion constant D…T. Muller, W. Selke·Jan 20, 1999SaveLearn
Dispersion of passive tracers in velocity field with non delta-correlated noiseThe diffusive properties in velocity fields whose small scales are parameterized by non δ-correlated noise is investigated using multiscale technique. The analytical expression of the eddy…P. Castiglione, A. Crisanti·Jan 20, 1999SaveLearn
Equivalent Linear Two-Body Equations for Many-Body SystemsA method has been developed for obtaining equivalent linear two-body equations (ELTBE) for the system of many (N) bosons using the variational principle. The method has been applied to the…Alexander L. Zubarev, Yeong E. Kim·Jan 19, 1999SaveLearn
From the magnetic-field-driven transitions to the zero-field transition in two-dimensionsFor more than a decade it was widely accepted that two-dimensional electrons are insulating at zero temperature and at zero magnetic-field. Experimentally it was demonstrated that, when placed in a…Y. Hanein, D. Shahar, Hadas Shtrikman et al.·Jan 19, 1999SaveLearn
The Extended Coupled Cluster Treatment of Correlations in Quantum MagnetsThe spin-half XXZ model on the linear chain and the square lattice are examined with the extended coupled cluster method (ECCM) of quantum many-body theory. We are able to describe both the…J. Rosenfeld, N. E. Ligterink, R. F. Bishop·Jan 19, 1999SaveLearn
The effect of temperature jumps during polymer crystallizationTemperature changes during the growth of lamellar polymer crystals give rise to steps on the surface of the crystals. It has recently been suggested that these steps could provide important insights…Jonathan Doye, Daan Frenkel·Jan 19, 1999SaveLearn
Asymptotic temperature dependence of the superfluid density in liquid 4HeIn a modified ideal Bose gas model we derive an expression for the temperature dependence of the superfluid fraction in liquid 4He. This expression leads to a fit formula for the asymptotic…Torsten Fliessbach·Jan 19, 1999SaveLearn
Theory of excitations of the condensate and non-condensate at finite temperaturesWe give an overview of the current theory of collective modes in trapped atomic gases at finite temperatures, when the dynamics of the condensate and non-condensate must both be considered. A simple…Allan Griffin·Jan 18, 1999SaveLearn
Spin relaxation of conduction electronsProspect of building electronic devices in which electron spins store and transport information has revived interest in the spin relaxation of conduction electrons. Since spin-polarized currents…Jaroslav Fabian, S. Das Sarma·Jan 18, 1999SaveLearn
Current self-oscillations, spikes and crossover between charge monopole and dipole waves in semiconductor superlatticesSelf-sustained current oscillations in weakly-coupled superlattices are studied by means of a self-consistent microscopic model of sequential tunneling including boundary conditions naturally.…David Sanchez, Miguel Moscoso, Luis L. Bonilla et al.·Jan 18, 1999SaveLearn