Excitations and S-matrix for su(3) spin chain combining 3 and $3*The associated Hamiltonian for a su(3) spin chain combining 3 and 3* representations is calculated. The ansatz equations for this chain are obtained and solved in the thermodynamic limit,…J. Abad, M. Ríos·Jan 14, 1998SaveLearn
Scaling Range and Cutoffs in Empirical FractalsFractal structures appear in a vast range of physical systems. A literature survey including all experimental papers on fractals which appeared in the six Physical Review journals (A-E and Letters)…Ofer Malcai, Daniel A. Lidar, Ofer Biham et al.·Jan 14, 1998SaveLearn
Dynamic percolation and Slow Relaxation in Glass-like MaterialsGlass-like materials are nonequilibrium systems where the relaxation time may exceed reasonable time scales of observations. In the present paper a dynamic percolation model is introduced in order to…A. Vazquez, O. Sotolongo-Costa·Jan 13, 1998SaveLearn
Periodic Modulation Induced Increase of Reaction Rates in Autocatalytic SystemsWe propose a new mechanism to increase the reactions ratesin multistable autocatalytic systems. The mechanism is based upon the possibility for the enhancement of the response of the system due to…T. Alarcon, A. Perez-Madrid, J. M. Rubi·Jan 13, 1998SaveLearn
Stochastic Resonance in Nonpotential SystemsWe propose a method to analytically show the possibility for the appearance of a maximum in the signal-to-noise ratio in nonpotential systems. We apply our results to the FitzHugh-Nagumo model under…T. Alarcon, A. Perez-Madrid, J. M. Rubi·Jan 13, 1998SaveLearn
Ring vortex destabilization in supersaturated 3He-4He liquid mixtures at low temperaturesThe effect of ring vortices on the destabilization of supersaturated liquid helium mixtures at very low temperatures is investigated as a function of pressure. We have found that large ring vortices…D. M. Jezek, M. Pi, M. Barranco et al.·Jan 13, 1998SaveLearn
Skyrmion in a real magnetic filmSkyrmions are the magnetic defects in an ultrathin magnetic film, similar to the bubble domains in the thicker films. Even weak uniaxial anisotropy determines its radius unambiguously. We consider…Ar. Abanov, V. L. Pokrovsky·Jan 13, 1998SaveLearn
Persistent Currents and Magnetization in two-dimensional Magnetic Quantum SystemsPersistent currents and magnetization are considered for a two-dimensional electron (or gas of electrons) coupled to various magnetic fields. Thermodynamic formulae for the magnetization and the…Jean Desbois, Stephane Ouvry, Christophe Texier·Jan 12, 1998SaveLearn
The Quantum Hall Effect in Quasi-1D ConductorsThe theory and experiments showing Quantum Hall effect in the quasi-one-dimensional conductors of the Bechgaard salts family are briefly reviewed. The sign reversals observed under some experimental…G. Montambaux, D. Zanchi·Jan 12, 1998SaveLearn
Negative Electric Current in SemiconductorsElectric current in semiconductors is considered as a function of time. Nonequilibrium fluctuations of the current are studied for strongly nonuniform samples. It is demonstrated that at special…V. I. Yukalov, E. P. Yukalova·Jan 12, 1998SaveLearn
Spectral Flow and the Dynamics of Dislocations in Charge Density WavesThe spectral flow in the cores of moving dislocations is found to play an important role in the dynamics and transport of charge density wave (CDW) by significantly modifying the hydrodynamic…Masahiko Hayashi·Jan 12, 1998SaveLearn
Bloch electrons in a Jahn-Teller crystal and an orbital-density-wave state due to the Berry phaseThe effect of the Berry phase is included explicitly in the wavefunction describing conduction electrons in a crystal composed of periodically arrayed Jahn-Teller centers that have conically…H. Koizumi, T. Hotta, Y. Takada·Jan 12, 1998SaveLearn
Stochastic Diagrams for Critical Point SpectraA new technique for calculating the time-evolution, correlations and steady state spectra for nonlinear stochastic differential equations is presented. To illustrate the method, we consider examples…S. Chaturvedi, P. D. Drummond·Jan 9, 1998SaveLearn
Dynamics of Bose condensed gases in highly deformed trapsWe provide a unified investigation of normal modes and sound propagation at zero temperature in Bose condensed gases confined in highly asymmetric harmonic traps and interacting with repulsive…S. Stringari·Jan 8, 1998SaveLearn
Stick-slip Transition in the Scalar Arching ModelWhen some granular material contained into a silo is pushed upwards with a piston, an irregular stick-slip motion of the system of grains is observed. We show how one can adapt the `Scalar Arching…Philippe Claudin, Jean-Philippe Bouchaud·Jan 7, 1998SaveLearn
Monte Carlo simulation of magnetization reversal via domain-wall motion in Fe sesquilayers on W(110)Iron sesquilayers are ultrathin films with coverages between one and two atomic monolayers. They consist of an almost defect-free monolayer with compact islands of a second atomic layer on top. This…M. Kolesik, M. A. Novotny, Per Arne Rikvold·Jan 7, 1998SaveLearn
Periodic features in the Dynamic Structure Factor of the Quasiperiodic Period-doubling LatticeWe present an exact real-space renormalization group (RSRG) method for evaluating the dynamic structure factor of an infinite one-dimensional quasiperiodic period-doubling (PD) lattice. We observe…Anathnath Ghosh, S. N. Karmakar·Jan 7, 1998SaveLearn
Plasma instability and amplification of electromagnetic waves in low-dimensional electron systemsA general electrodynamic theory of a grating coupled two dimensional electron system (2DES) is developed. The 2DES is treated quantum mechanically, the grating is considered as a periodic system of…S. A. Mikhailov·Jan 7, 1998SaveLearn
Physical nature of all the electronic states in the Thue-Morse chainWe present an analytical method for finding all the electronic eigenfunctions and eigenvalues of the aperiodic Thue-Morse lattice. We prove that this system supports only extended electronic states…Anathnath Ghosh, S. N. Karmakar·Jan 7, 1998SaveLearn
A divergent correlation length in off-equilibrium glassesIn off-equilibrium dynamics we define a dynamical correlation length which is proportional to the size of the region in which the atoms move in a correlated way. General arguments indicate that this…Giorgio Parisi·Jan 6, 1998SaveLearn
Hydrodynamic damping in trapped Bose gasesGriffin, Wu and Stringari have derived the hydrodynamic equations of a trapped dilute Bose gas above the Bose-Einstein transition temperature. We give the extension which includes hydrodynamic…T. Nikuni, A. Griffin·Jan 6, 1998SaveLearn
Role of quasiparticles in the growth of a trapped Bose-Einstein condensateA major extension of the model of condensate growth introduced by us is made to take account of the evolution of the occupations of lower trap levels (quasiparticles) by scattering processes, and of…C. W. Gardiner, M. D. Lee, R. J. Ballagh et al.·Jan 5, 1998SaveLearn
Shadow Bands and Tunneling Magnetoresistance in Itinerant Electron FerromagnetsIn itinerant electron ferromagnets spectral weight is transferred at finite temperatures from quasiparticle peaks located at majority and minority-spin band energies to shadow-band peaks. For a given…A. H. MacDonald, T. Jungwirth, M. Kasner·Jan 5, 1998SaveLearn
The charge density of semiconductors in the GW approximationWe present a method to calculate the electronic charge density of periodic solids in the GW approximation, using the space-time method. We investigate for the examples of silicon and germanium to…Martin M. Rieger, R. W. Godby·Jan 5, 1998SaveLearn
Effect of electron corelation on superconducting pairing symmetryThe role of electron correlation on different pairing symmetries are discussed in details where the electron correlation has been treated within the slave boson formalism. It is shown that for a pure…Manidipa Mitra, Haranath Ghosh, S. N. Behera·Jan 2, 1998SaveLearn