High-field AFMR in single-crystalline La0.95Sr0.05MnO3: Experimental evidence for the existence of a canted magnetic structureHigh-field antiferromagnetic-resonance (AFMR) spectra were obtained in the frequency range 60 GHz < ν< 700 GHz and for magnetic fields up to 8 T in twin-free single crystals of…A. Pimenov, M. Biberacher, D. Ivannikov et al.·Feb 28, 2000SaveLearn
Intermittent implosion and pattern formation of trapped Bose-Einstein condensates with attractive interactionThe collapsing dynamics of a trapped Bose-Einstein condensate (BEC) with attractive interaction are revealed to exhibit two previously unknown phenomena. During the collapse, BEC undergoes a series…Hiroki Saito, Masahito Ueda·Feb 25, 2000SaveLearn
Mechanical detection of nuclear spin relaxation in a micron-size crystalA room temperature nuclear magnetic resonance force microscope (MRFM), fitted in a 1Tesla electromagnet, is used to measure the nuclear spin relaxation of 1H in a micron-size (70ng) crystal of…O. Klein, V. V. Naletov, H. Alloul·Feb 25, 2000SaveLearn
The effect of strain on the adsorption of CO on Pd(100)We study how the binding energy, the vibrational frequencies and the adsorption isotherm of CO on Pd(100) are modified when the solid is subject to uniform strain. The parameters controlling the…M. W. Wu, H. Metiu·Feb 25, 2000SaveLearn
Super-radiant light scattering from trapped Bose Einstein condensatesWe propose a new formulation for atomic side mode dynamics from super-radiant light scattering of trapped atoms. A detailed analysis of the recently observed super-radiant light scattering from…Ozgur E. Mustecaplioglu, L. You·Feb 25, 2000SaveLearn
How to mode-lock an atom laserWe consider a possible technique for mode-locking an atom laser, based on the generation of a dark soliton in a ring-shaped Bose-Einstein condensate, with repulsive atomic interactions. The soliton…Peter D. Drummond, Antonios Eleftheriou, Kerson Huang et al.·Feb 24, 2000SaveLearn
Snake orbits and related magnetic edge statesWe study the electron motion near magnetic field steps at which the strength and/or sign of the magnetic field changes. The energy spectrum for such systems is found and the electron states (bound…J. Reijniers, F. M. Peeters·Feb 24, 2000SaveLearn
Wealth condensation in a simple model of economyWe introduce a simple model of economy, where the time evolution is described by an equation capturing both exchange between individuals and random speculative trading, in such a way that the…Jean-Philippe Bouchaud, Marc Mezard·Feb 24, 2000SaveLearn
Random-mass Dirac fermions in an imaginary vector potential: Delocalization transition and localization lengthOne dimensional system of Dirac fermions with a random-varying mass is studied by the transfer-matrix methods which we developed recently. We investigate the effects of nonlocal correlation of the…Koujin Takeda, Ikuo Ichinose·Feb 24, 2000SaveLearn
Temperature effect in the Casimir attraction of a thin metal filmThe Casimir effect for conductors at arbitrary temperatures is theoretically studied. By using the analytical properties of the Green functions and applying the Abel-Plan formula to Lifshitz's…V. N. Dubrava, V. A. Yampol'skii·Feb 24, 2000SaveLearn
Three-body recombination in Bose gases with large scattering lengthAn effective field theory for the three-body system with large scattering length is applied to three-body recombination to a weakly-bound s-wave state in a Bose gas. Our model independent analysis…P. F. Bedaque, E. Braaten, H. -W. Hammer·Feb 23, 2000SaveLearn
Single and Paired Point Defects in a 2D Wigner CrystalUsing the path-integral Monte Carlo method, we calculate the energy to form single and pair vacancies and interstitials in a two-dimensional Wigner crystal of electrons. We confirm that the…Ladir Cândido, Philip Phillips, D. M. Ceperley·Feb 23, 2000SaveLearn
Collective Phenonema in the Interaction of Radiation with MatterThe aim of this communication is to present in a concentrated form the main ideas of a method, developed by the author, for treating strongly nonequilibrium collective phenomena typical of the…V. I. Yukalov·Feb 23, 2000SaveLearn
Numerical analyses of the nonequilibrium electron transport through the Kondo impurity beside the Toulouse pointNonequilibrium electron transport through the Kondo impurity is investigated numerically for the system with twenty conduction-electron levels. The electron current under finite voltage drop is…Yoshihiro Nishiyama·Feb 23, 2000SaveLearn
Many Body Diffusion and Interacting Electrons in a Harmonic ConfinementWe present numerically exact energy estimates for two-dimensional electrons in a parabolic confinement. By application of an extension of the recently introduced many-body diffusion algorithm, the…F. Luczak, F. Brosens, J. T. Devreese et al.·Feb 22, 2000SaveLearn
Gaussian to Exponential Crossover in the Attenuation of Polarization Echoes in NMRAn ingenious pulse sequence devised by S. Zhang, B. H. Meier, and R. R. Ernst (Phys. Rev. Lett. 69, 2149 (1992)) reverses the time evolution (``spin diffusion'') of the local…Gonzalo Usaj, Horacio M. Pastawski, Patricia R. Levstein·Feb 21, 2000SaveLearn
New way to achieve chaotic synchronization in spatially extended systemsWe study the spatio-temporal behavior of simple coupled map lattices with periodic boundary conditions. The local dynamics is governed by two maps, namely, the sine circle map and the logistic map…Bikash Chandra Gupta, P. A. Sreeram, S. B. Lee·Feb 21, 2000SaveLearn
Modes of counterion density-fluctuations and counterion-mediated attractions between like-charged fluid membranesCounterion-mediated attractions between like-charged fluid membranes are long-ranged and non-pairwise additive at high temperatures. At zero temperature, however, they are pairwise additive and decay…Bae-Yeun Ha·Feb 21, 2000SaveLearn
Quenched Averaged Correlation Functions of the Random MagnetsIt is shown that the ratios of the quenched averaged three and four-point correlation functions of the local energy density operator to the connected ones in the random-bond Ising model approach…M. Reza Rahimi Tabar·Feb 19, 2000SaveLearn
Linear and nonlinear susceptibilities of a decoherent two-level systemThe linear and nonlinear dynamical susceptibilities of a two level system are calculated as it undergoes a transition to a decoherent state. Analogously to the Glover-Tinkham-Ferrell sum rule of…Gregory Levine·Feb 19, 2000SaveLearn
Delocalization of two-particle ring near the Fermi level of 2d Anderson modelWe study analytically and numerically the problem of two particles with a long range attractive interaction on a two-dimensional (2d) lattice with disorder. It is shown that below some critical…J. Lages, D. L. Shepelyansky·Feb 18, 2000SaveLearn
Order-disorder model of phase transitions in the DMAGaS-DMAAlS family crystalsA four-state model is proposed for description of the sequence of phase transitions in ferroelectric crystals of DMAGaS and DMAAlS type. The ordering processes in the subsystems of DMA groups are…I. V. Stasyuk, O. V. Velychko·Feb 18, 2000SaveLearn
Dynamics of Excited Electrons in Copper: Role of Auger ElectronsWithin a theoretical model based on the Boltzmann equation, we analyze in detail the structure of the unusual peak recently observed in the relaxation time in Cu. In particular, we discuss the role…R. Knorren, G. Bouzerar, K. H. Bennemann·Feb 18, 2000SaveLearn
Current bistability and hysteresis in strongly correlated quantum wiresNonequilibrium transport properties are determined exactly for an adiabatically connected single channel quantum wire containing one impurity. Employing the Luttinger liquid model with interaction…R. Egger, H. Grabert, A. Koutouza et al.·Feb 18, 2000SaveLearn
Ab initio Hartree-Fock Born effective charges of LiH, LiF, LiCl, NaF, and NaClWe use the Berry-phase-based theory of macroscopic polarization of dielectric crystals formulated in terms of Wannier functions, and state-of-the-art Gaussian basis functions, to obtain benchmark ab…Alok Shukla·Feb 18, 2000SaveLearn