Bosonization of Fermi LiquidsWe consider systems of non-relativistic, interacting electrons at finite density and zero temperature in d = 2, 3, ... dimensions. Our main concern is to characterize those systems that, under the…Juerg Froehlich, Roland Goetschmann·Jun 14, 1996SaveLearn
The Magnus force in superfluids and superconductorsThe forces on the vortex, transverse to its velocity, are considered. In addition to the superfluid Magnus force from the condensate (superfluid component), there are transverse forces from thermal…E. B. Sonin·Jun 14, 1996SaveLearn
Macrodynamics of Disordered and Frustrated SystemsIt is shown how the macroscopic non-equilibrium dynamics of a class of systems whose microscopic stochastic dynamics involves disordered and frustrated but range-free interactions can be well…D. Sherrington, A. C. C. Coolen, S. N. Laughton·Jun 14, 1996SaveLearn
A model for the compaction of granular mediaWe introduce a lattice model, in which frustration plays a crucial role, to describe relaxation properties of granular media. We show Monte Carlo results for compaction in the presence of vibrations…Mario Nicodemi, Antonio Coniglio, Hans J. Herrmann·Jun 14, 1996SaveLearn
Two dimensional bulk bands and surfaces resonances originated from (100) surfaces of III-V semiconductor compoundsWe have calculated the electronic band structure of the (100) surface of the III--V zinc blende semiconductor compounds, using the standard tight binding method and the surface Green's function…Daniel Olguin, Rafael Baquero·Jun 14, 1996SaveLearn
Calculation of Universal Amplitude Ratios in three-loop orderFor the universality class of three-dimensional Ising systems the ratio of the high- and low-temperature amplitudes for the correlation length and for the susceptibility are universal quantities.…Christoph Gutsfeld, Jens Kuester, Gernot Muenster·Jun 13, 1996SaveLearn
Nearly critical ground state of LaCuO2.5Using a combination of analytical techniques and Quantum Monte Carlo simulations we investigate the coupled spin ladder system LaCuO2.5. At a critical ratio of the interladder to intraladder coupling…Matthias Troyer, M. E. Zhitomirsky, Kazuo Ueda·Jun 13, 1996SaveLearn
Self-Consistent Model of Polymerization-Induced Phase SeparationWe propose an exactly solvable self-consistent kinetic model of polymerization-induced phase separation (PIPS) via spinodal decomposition. Using modified Cahn-Hilliard and Glotzer-Coniglio theories…Valeriy V. Ginzburg, Noel A. Clark·Jun 13, 1996SaveLearn
Effect of disorder on the magnetic and transport properties of La1-xSrxMnO3We study a simplified model of the electronic structure of compounds of the type of La1-xSrxMnO3. The model represents each Mn4+ ion by a spin S=1/2, on which an electron can be added…R. Allub, B. Alascio·Jun 13, 1996SaveLearn
Anomalous Dimension and Spatial Correlations in a Point-Island ModelWe examine the island size distribution function and spatial correlation function of a model for island growth in the submonolayer regime in both 1 and 2 dimensions. In our model the islands do not…Ji Li, A. G. Rojo, Leonard M. Sander·Jun 13, 1996SaveLearn
d-Wave Order Parameter in Bi2212 from a Phenomenological Model of High Tc CupratesA phenomenological lattice model of high Tc cuprates including order parameter phase fluctuations is considered within the BCS approximation, to interpret the experimental data from ARPES…Biplab Chattopadhyay·Jun 13, 1996SaveLearn
Kosterlitz-Thouless Transition and Short Range Spatial Correlations in an Extended Hubbard ModelWe study the competition between intersite and local correlations in a spinless two-band extended Hubbard model by taking an alternative limit of infinite dimensions. We find that the intersite…Qimiao Si, J. Lleweilun Smith·Jun 13, 1996SaveLearn
New magnetic coherence effect in superconducting La2-xSrxCuO4We have used inelastic neutron scattering to examine the magnetic fluctuations at intermediate frequencies in the simplest high temperature superconductor, La2-xSrxCu4. The suppression of…T. E. Mason, A. Schroder, G. Aeppli et al.·Jun 12, 1996SaveLearn
Electronic and Magnetic States in the Giant Magneto-resistive CompoundsThe paramagnetic insulator to ferromagnetic metal transition in Lanthanum manganites and the associated magnetoresistive phenomena is treated by considering the localization due to random hopping…C. M. Varma·Jun 12, 1996SaveLearn
Anomalous density dependence of static friction in sandWe measured experimentally the static friction force Fs on the surface of a glass rod immersed in dry sand. We observed that Fs is extremely sensitive to the closeness of packing of grains. A…Viktor K. Horváth, Imre M. Jánosi, Péter J. Vella·Jun 12, 1996SaveLearn
Theory of finite temperature crossovers near quantum critical points close to, or above, their upper-critical dimensionA systematic method for the computation of finite temperature (T) crossover functions near quantum critical points close to, or above, their upper-critical dimension is devised. We describe the…Subir Sachdev·Jun 12, 1996SaveLearn
A new perspective on the Holstein polaron problemThe single-polaron band structure of the Holstein model in one and two dimensions is studied using a new form of resummed strong-coupling perturbation theory. Well converged results are obtained for…Walter Stephan·Jun 12, 1996SaveLearn
Universal Formulae for Percolation ThresholdsA power law is postulated for both site and bond percolation thresholds. The formula writes pc=p0[(d-1)(q-1)]-ad\ b, where d is the space dimension and q the coordination number. All…Serge Galam, Alain Mauger·Jun 12, 1996SaveLearn
Equation of State for Exclusion Statistics in a Harmonic WellWe consider the equations of state for systems of particles with exclusion statistics in a harmonic well. Paradygmatic examples are noninteracting particles obeying ideal fractional exclusion…Serguei B. Isakov, Stéphane Ouvry·Jun 12, 1996SaveLearn
Temperature and Pressure Effects on the Resistivity of the Manganese OxidesThe temperature and pressure effects on the resistivity of the manganese oxides are studied analytically via the Kondo lattice model with a strong Hund's coupling. We obtain analytically the…Hae-Young Kee, Jongbae Hong·Jun 12, 1996SaveLearn
Microscopic Derivation of Non-Markovian Thermalization of a Brownian ParticleIn this paper, the first microscopic approach to the Brownian motion is developed in the case where the mass density of the suspending bath is of the same order of magnitude as that of the Brownian…Lydéric Bocquet, Jarosław Piasecki·Jun 12, 1996SaveLearn
Metastability and Glassy Behavior of a Driven Flux-Line LatticeStrong metastability and history dependence are observed in DC and pulsed transport studies of flux-line lattices in 2H-NbSe2, leading to the identification of two distinct states of the lattice…W. Henderson, E. Y. Andrei, M. J. Higgins et al.·Jun 11, 1996SaveLearn
Stability Conditions and the Single Mode Approximation in FQHEA thermodynamic stability criterion for the spontaneous breaking of the translation invariance of many particle systems is derived. It simply requires the positive character of the wavevector…Alejandro Cabo, Aurora Perez Martinez·Jun 11, 1996SaveLearn
Quantized hydrodynamic model and the dynamic structure factor for a trapped Bose gasWe quantize the recent hydrodynamic analysis of Stringari for the low-energy collective modes of a trapped Bose gas at T=0. This is based on the time-dependent Gross-Pitaevskii equation, but omits…Wen-Chin Wu, A. Griffin·Jun 11, 1996SaveLearn
On Magnetic Impurities in Gapless Fermi SystemsIn ordinary metals, antiferromagnetic exchange between conduction electrons and a magnetic impurity leads to screening of the impurity spin below the Kondo temperature, TK. In systems such as…L. S. Borkowski·Jun 11, 1996SaveLearn