The rheology of field-responsive suspensionsWe present some aspects of the rheology of field-responsive suspensions, a class of field-responsive liquid matter systems possessing the ability to undergo significant changes in their strength upon…J. M. Rubí, J. M. G. Vilar·Sep 24, 1999SaveLearn
Phase separation, percolation and giant isotope effect in manganitesPhase separation and a tendency to form inhomogeneous structures seems to be a generic property of systems with strongly correlated electrons. After shortly summarising the existing theoretical…D. Khomskii·Sep 23, 1999SaveLearn
Charge inversion in DNA-amphiphile complexes: Possible application to gene therapyWe study a complex formation between the DNA and cationic amphiphilic molecules. As the amphiphile is added to the solution containing DNA, a cooperative binding of surfactants to the DNA molecules…P. S. Kuhn, Y. Levin, M. C. Barbosa·Sep 23, 1999SaveLearn
Magnetization-controlled spin transport in DyAs/GaAs layersElectrical transport properties of DyAs epitaxial layers grown on GaAs have been investigated at various temperatures and magnetic fields up to 12T. The measured longitudinal resistances show two…J. M. Mao, M. E. Zudov, R. R. Du et al.·Sep 23, 1999SaveLearn
Acoustic Energy and Momentum in a Moving MediumBy exploiting the mathematical analogy between the propagation of sound in a non-homogeneous potential flow and the propagation of a scalar field in a background gravitational field, various wave…Michael Stone·Sep 21, 1999SaveLearn
Iordanskii Force and the Gravitational Aharonov-Bohm effect for a Moving VortexI discuss the scattering of phonons by a vortex moving with respect to a superfluid condensate. This allows us to test the compatibility of the scattering-theory derivation of the Iordanskii force…Michael Stone·Sep 21, 1999SaveLearn
Electron locking in semiconductor superlatticesWe describe a novel state of electrons and phonons arising in semiconductor superlattices (SSL) due to strong electron-phonon interactions. These states are characterized by a localization of phonons…F. V. Kusmartsev, H. S. Dhillon·Sep 21, 1999SaveLearn
The energy spectrum of complex periodic potentials of the Kronig-Penney typeWe consider a complex periodic PT-symmetric potential of the Kronig-Penney type, in order to elucidate the peculiar properties found by Bender et al. for potentials of the form V=i( x)2N+1,…H. F. Jones·Sep 20, 1999SaveLearn
Electron States in a Staircase Infinitely Deep Well in a Magnetic FieldThe electron states in a size-quantaized coated semiconductor wire in a uniform magnetic field applied parallel to the wire axis is considered. The wave functions are found and the equation for…M. M. Aghasyan A. A. Kirakosyan·Sep 20, 1999SaveLearn
Band structure of local pairs. Mathematical toolsA system of strongly interacting fermions in a solid state is discussed. A structure of singlet and triplet coupled 2-particle states and their excitation spectra are investigated. It is shown that…S. G. Rubin·Sep 18, 1999SaveLearn
Calculation of Neel temperature for S=1/2 quasi-one-dimensional Heisenberg antiferromagnetsIsotropic S=1/2 quasi-one-dimensional antiferromagnets are considered within the bosonization method. The 1/zp-corrections to the interchain mean-field theory (zp is the number of nearest neighbors…V. Yu. Irkhin, A. A. Katanin·Sep 17, 1999SaveLearn
Slow 4He Quenches Produce Fuzzy, Transient VorticesWe examine the Zurek scenario for the production of vortices in quenches of liquid 4He in the light of recent experiments. Extending our previous results to later times, we argue that short…R. J. Rivers·Sep 16, 1999SaveLearn
High-field transport properties of bulk Si: A test for the Fokker-Planck approachHigh electric-field transport parameters are calculated using an analytical Fokker-Planck approach (FPA), where transport is modeled as a drift-diffusion process in energy space. We have applied the…F. Comas, Nelson Studart·Sep 16, 1999SaveLearn
The spin-1/2 transverse XX chain with regularly alternating bonds and fieldsWe use continued fractions for a study of the thermodynamic properties of the periodic nonuniform spin-1/2 isotropic XY chain in a non-random/random (Lorentzian) transverse field. The obtained…Oleg Derzhko, Johannes Richter, Oles' Zaburannyi·Sep 16, 1999SaveLearn
Worse fluctuation method for fast Value-at-Risk estimatesWe show how one can actually take advantage of the strongly non-Gaussian nature of the fluctuations of financial assets to simplify the calculation of the Value-at-Risk of complex non linear…Jean-Philippe Bouchaud, Marc Potters·Sep 16, 1999SaveLearn
Microwave study of quantum n-disk scatteringWe describe a wave-mechanical implementation of classically chaotic n-disk scattering based on thin 2-D microwave cavities. Two, three, and four-disk scattering are investigated in detail. The…Wentao Lu, Lorenza Viola, Kristi Pance et al.·Sep 16, 1999SaveLearn
Introduction to Multicanonical Monte Carlo SimulationsMonte Carlo simulation with a-priori unknown weights have attracted recent attention and progress has been made in understanding (i) the technical feasibility of such simulations and (ii)…Bernd A. Berg·Sep 15, 1999SaveLearn
Internal Diffusion-Limited Aggregation: Parallel Algorithms and ComplexityThe computational complexity of internal diffusion-limited aggregation (DLA) is examined from both a theoretical and a practical point of view. We show that for two or more dimensions, the problem of…Cristopher Moore, Jonathan Machta·Sep 15, 1999SaveLearn
Lexicon of Topological Defects in He-3 SuperfluidsDefects in the multi-dimensional macroscopic quantum field of the He-3 superfluids are localized objects with a topological charge and are topologically stable. They include point-like objects,…V. B. Eltsov, M. Krusius·Sep 15, 1999SaveLearn
Charge Fluctuations in the Two-Dimensional One-Component PlasmaWe study, via computer simulations, the fluctuations in the net electric charge, in a two dimensional one component plasma (OCP) with uniform background charge density -e ρ, in a region Λ inside…D. Levesque, J. -J. Weis, J. L. Lebowitz·Sep 14, 1999SaveLearn
Finite-Size Scaling in Two-dimensional Continuum Percolation ModelsWe test the universal finite-size scaling of the cluster mass order parameter in two-dimensional (2D) isotropic and directed continuum percolation models below the percolation threshold by computer…Van Lien Nguyen, Enrique Canessa·Sep 14, 1999SaveLearn
The partition function for "composite particles"We calculate the partition function for "composite particles". For any finite number of states d, and in the following two cases: 1)all states have the same energy, 2)the energy is linearly…M. Bergère·Sep 13, 1999SaveLearn
On non-Riemannian geometry of twisted nematic liquid crystalsA teleparallel geometrical description of the nematic phases of liquid crystals is proposed.In the case of the twisted geometry of nematics Cartan torsion is given by a spatial helical form which…L. C. Garcia de Andrade·Sep 13, 1999SaveLearn
Path integral Monte Carlo simulation of helium at negative pressuresPath integral Monte Carlo (PIMC) simulations of liquid helium at negative pressure have been carried out for a temperature range from the critical temperature to below the superfluid transition. We…G. H. Bauer, D. M. Ceperley, Nigel Goldenfeld·Sep 11, 1999SaveLearn
Tunnelling of topological line defects in strongly coupled superfluidsThe geometric theory of vortex tunnelling in superfluid liquids is developed. Geometry rules the tunnelling process in the approximation of an incompressible superfluid, which yields the identity of…Uwe R. Fischer·Sep 10, 1999SaveLearn