Continuous Elastic Phase Transitions in Pure and Disordered CrystalsWe review the theory of second--order (ferro--)elastic phase transitions, where the order parameter consists of a certain linear combination of strain tensor components, and the accompanying soft…F. Schwabl, U. C. Täuber·Jul 4, 1996SaveLearn
On Metal-Insulator Transitions due to Self-DopingWe investigate the influence of an unoccupied band on the transport properties of a strongly correlated electron system. For that purpose, additional orbitals are coupled to a Hubbard model via…Stefan Blawid, Hoangh Anh Tuan, Takashi Yanagisawa et al.·Jul 4, 1996SaveLearn
Exponents appearing in heterogeneous reaction-diffusion models in one dimensionWe study the following 1D two-species reaction diffusion model : there is a small concentration of B-particles with diffusion constant DB in an homogenous background of W-particles with diffusion…Cécile Monthus·Jul 4, 1996SaveLearn
Traveling-Wave ChemotaxisA simple model is studied for the chemotactic movement of biological cells in the presence of a periodic chemical wave. It incorporates the feature of adaptation that may play an important role in…Raymond E. Goldstein·Jul 4, 1996SaveLearn
On the Kinetics of Multi-dimensional FragmentationWe present two classes of exact solutions to a geometric model which describes the kinetics of fragmentation of d-dimensional hypercuboid-shaped objects. The first class of exact solutions is…P. Singh, M. K. Hassan·Jul 4, 1996SaveLearn
Equilibrium properties of the Ising frustrated lattice gasWe study the equilibrium properties of an Ising frustrated lattice gas with a mean field replica approach. This model bridges usual Spin Glasses and a version of Frustrated Percolation…Jeferson J. Arenzon, Mario Nicodemi, Mauro Sellitto·Jul 4, 1996SaveLearn
Monte Carlo simulation of a two-dimensional continuum Coulomb gasWe study the classical two-dimensional Coulomb gas model for thermal vortex fluctuations in thin superconducting/superfluid films by Monte Carlo simulation of a grand canonical vortex ensemble…Jack Lidmar, Mats Wallin·Jul 4, 1996SaveLearn
Fractal formation and ordering in Random Sequential AdsorptionWe study the kinetics of random sequential adsorption of a mixture of particles with continuous distribution of sizes for different deposition rules. It appears in the long time limit the resulting…M. K. Hassan·Jul 3, 1996SaveLearn
How to derive a protein folding potential? A new approach to the old problemIn this paper we introduce a novel method of deriving a pairwise potential for protein folding. The potential is obtained by optimization procedure, which simultaneously maximizes the energy gap for…L. A. Mirny, E. I. Shakhnovich·Jul 3, 1996SaveLearn
Velocity Selection for Propagating Fronts in SuperconductorsUsing the time-dependent Ginzburg-Landau equations we study the propagation of planar fronts in superconductors, which would appear after a quench to zero applied magnetic field. Our numerical…S. John Di Bartolo, Alan T. Dorsey·Jul 3, 1996SaveLearn
Improved Power Counting and Fermi Surface RenormalizationThe naive perturbation expansion for many-fermion systems is infrared divergent. One can remove these divergences by introducing counterterms. To do this without changing the model, one has to solve…Manfred Salmhofer·Jul 3, 1996SaveLearn
Laplacian growth as one-dimensional turbulenceA new model of Laplacian stochastic growth is formulated using conformal mappings. The model describes two growth regimes, stable and turbulent, separated by a sharp phase transition. The first few…M. B. Hastings, L. S. Levitov·Jul 3, 1996SaveLearn
Medium-range interactions and crossover to classical critical behaviorWe study the crossover from Ising-like to classical critical behavior as a function of the range R of interactions. The power-law dependence on R of several critical amplitudes is calculated from…Erik Luijten, Henk W. J. Blöte, Kurt Binder·Jul 3, 1996SaveLearn
Quantum Ergodicity and Localization in Conservative Systems: the Wigner Band Random Matrix ModelFirst theoretical and numerical results on the global structure of the energy shell, the Green function spectra and the eigenfunctions, both localized and ergodic, in a generic conservative quantum…G. Casati, B. V. Chirikov, I. Guarneri et al.·Jul 3, 1996SaveLearn
Point interactions in a stripWe study the behavior of a quantum particle confined to a hard--wall strip of a constant width in which there is a finite number N of point perturbations. Constructing the resolvent of the…P. Exner, R. Gawlista, P. Šeba et al.·Jul 3, 1996SaveLearn
Point interaction in dimension two and three as models of small scatterersIn addition to the conventional renormalized--coupling--constant picture, point interactions in dimension two and three are shown to model within a suitable energy range scattering on localized…P. Exner, P. Šeba·Jul 3, 1996SaveLearn
Manifestation of the Hofstadter butterfly in far-infrared absorptionThe far-infrared absorption of a two-dimensional electron gas with a square-lattice modulation in a perpendicular constant magnetic field is calculated self-consistently within the Hartree…Vidar Gudmundsson, Rolf R. Gerhardts·Jul 3, 1996SaveLearn
Quantum Hall quarks or Short distance physics of quantized Hall fluidsIn order to obtain a local description of the short distance physics of fractionally quantized Hall states for realistic (e.g. Coulomb) interactions, I propose to view the zeros of the ground state…Martin Greiter·Jul 3, 1996SaveLearn
Novel Correlations in Arbitrary DimensionsWe present a new three dimensional many-body Hamiltonian with three-body and five-body interactions. We obtain the exact ground state as well as some excited states of this Hamiltonian for arbitrary…Pijush K. Ghosh·Jul 2, 1996SaveLearn
Generalized Dynamic Scaling for Critical RelaxationsThe dynamic relaxation process for the two dimensional Potts model at criticality starting from an initial state with very high temperature and arbitrary magnetization is investigated with Monte…B. Zheng·Jul 2, 1996SaveLearn
Gap States in Dilute Magnetic Alloy SuperconductorsWe study states in the superconducting gap induced by magnetic impurities using self-consistent quantum Monte Carlo with maximum entropy and formally exact analytic continuation methods. The magnetic…Woonki Chung, Mark Jarrell·Jul 2, 1996SaveLearn
Phase separation in the one-dimensional Hubbard modelThe Hartree-Fock ground-state phase diagram of the one-dimensional Hubbard model is calculated in the μ-U plane, restricted to phases with no charge density modulation, extending the results…J. H. Samson·Jul 2, 1996SaveLearn
Cooling rate effects in amorphous Silica: A Computer Simulation StudyUsing molecular dynamics computer simulations we investigate how in silica the glass transition and the properties of the resulting glass depend on the cooling rate with which the sample is cooled.…Katharina Vollmayr, Walter Kob, Kurt Binder·Jul 2, 1996SaveLearn
Thermoelectric Response of an Interacting Two-Dimensional Electron Gas in Quantizing Magnetic FieldWe present a discussion of the linear thermoelectric response of an interacting electron gas in a quantizing magnetic field. Boundary currents can carry a significant fraction of the net current…N. R. Cooper, B. I. Halperin, I. M. Ruzin·Jul 1, 1996SaveLearn
Theoretical study of hydrogen-covered diamond (100) surfaces: A chemical potential analysisThe bare and hydrogen-covered diamond (100) surfaces were investigated through pseudopotential density-functional calculations within the local-density approximation. Different coverages, ranging…Suklyun Hong, M. Y. Chou·Jul 1, 1996SaveLearn