The Debye-Waller Factor in solid 3He and 4HeThe Debye-Waller factor and the mean-squared displacement from lattice sites for solid 3He and 4He were calculated with Path Integral Monte Carlo at temperatures between 5 K and 35 K, and densities…E. W. Draeger, D. M. Ceperley·Oct 20, 1999SaveLearn
Magnetic strip waveguidesWe analyze the spectrum of the "local" Iwatsuka model, i.e. a two-dimensional charged particle interacting with a magnetic field which is homogeneous outside a finite strip and…Pavel Exner, Hynek Kovarik·Oct 20, 1999SaveLearn
Renormalized Theory of Infinitely Driven Lattice GasesWe use field theoretic renormalization group methods to study the critical behavior of a recently proposed Langevin equation for driven lattice gases under infinitely fast drive. We perform an…F. de los Santos, Miguel A. Muñoz·Oct 20, 1999SaveLearn
A scaling theory of 3D spinodal turbulenceA new scaling theory for spinodal decomposition in the inertial hydrodynamic regime is presented. The scaling involves three relevant length scales, the domain size, the Taylor microscale and the…V M Kendon·Oct 19, 1999SaveLearn
Zener transitions between dissipative Bloch bands. II: Current Response at Finite TemperatureWe extend, to include the effects of finite temperature, our earlier study of the interband dynamics of electrons with Markoffian dephasing under the influence of uniform static electric fields. We…Xian-Geng Zhao, Daniel W. Hone·Oct 19, 1999SaveLearn
A Generalized Ginzburg-Landau Approach to Second Harmonic GenerationWe develop a generalized Ginzburg-Landau theory for second harmonic generation (SHG) in magnets by expanding the free energy in terms of the order parameter in the magnetic phase and the…Debanand Sa, R. Valenti, C. Gros·Oct 19, 1999SaveLearn
Signatures of an intermediate 2d Coulomb phase at low temperaturesThe study of the ground state of spinless fermions in 2d disordered clusters (Phys. Rev. Lett. 83, 1826 (1999)) has suggested the existence of a new quantum phase for intermediate Coulomb…Giuliano Benenti, Xavier Waintal, Jean-Louis Pichard·Oct 18, 1999SaveLearn
Universal Selftrapping in Nonlinear Tight-binding LatticesWe show that nonlinear tight-binding lattices of different geometries and dimensionalities, display an universal selftrapping behavior. First, we consider the single nonlinear impurity problem in…C. A. Bustamante, M. I. Molina·Oct 18, 1999SaveLearn
Spectral Representation for the Effective Macroscopic Response of a Polycrystal: Application to Third-Order Nonlinear SusceptibilityErratum: In our paper, we show that the spectral representation for isotropic two-component composites also applies to uniaxial polycrystals. We have learned that this result was, in fact, first…S. Barabash, D. Stroud·Oct 15, 1999SaveLearn
Hydrodynamic Approach to Vortex Lifetime in Trapped Bose CondensatesWe study a vortex in a two-dimensional, harmonically trapped Bose-Einstein condensate at zero temperature. Through a variational calculation using a trial condensate wave function and a nonlinear…Emil Lundh, P. Ao·Oct 15, 1999SaveLearn
Magnetic field induced directional localization in a 2D rectangular latticeWe study the effect of a perpendicular uniform magnetic field on the dissipative conductivity of a rectangular lattice with anisotropic hopping, tx≠ ty . We show that the magnetic field may…Armelle Barelli, Jean Bellissard, Francisco Claro·Oct 14, 1999SaveLearn
Driven Tunneling: Chaos and DecoherenceChaotic tunneling in a driven double-well system is investigated in absence as well as in the presence of dissipation. As the constitutive mechanism of chaos-assisted tunneling, we focus on the…Peter Hanggi, Sigmund Kohler, Thomas Dittrich·Oct 13, 1999SaveLearn
Doping dependence of the Neel temperature in Mott-Hubbard antiferromagnets: Effect of vorticesThe rapid destruction of long-range antiferromagnetic order upon doping of Mott-Hubbard antiferromagnetic insulators is studied within a generalized Berezinskii-Kosterlitz-Thouless renormalization…Carsten Timm, K. H. Bennemann·Oct 13, 1999SaveLearn
Coupled-mode theory for Bose-Einstein condensatesWe apply the concepts of nonlinear guided-wave optics to a Bose-Einstein condensate (BEC) trapped in an external potential. As an example, we consider a parabolic double-well potential and derive…Elena A. Ostrovskaya, Yuri S. Kivshar, Mietek Lisak et al.·Oct 13, 1999SaveLearn
Designing emissive conjugated polymers with small optical gaps: a step towards organic polymeric infrared lasersWe show that chemical modification of the trans-polyacetylene structure that involves substitution of the backbone hydrogen atoms with conjugated side groups, leads to reduction of the backbone bond…Alok Shukla, Sumit Mazumdar·Oct 13, 1999SaveLearn
Dynamical Transverse Meissner Effect and Transition in Moving Bose GlassWe study moving periodic structures in presence of correlated disorder using renormalisation group. We find that the effect of disorder persists at all velocities resulting at zero temperature in a…Pascal Chauve, Pierre Le Doussal, Thierry Giamarchi·Oct 13, 1999SaveLearn
On modulational instability and energy localization in anharmonic lattices at finite energy densityThe localization of vibrational energy, induced by the modulational instability of the Brillouin-zone-boundary mode in a chain of classical anharmonic oscillators with finite initial energy density,…Yuriy A. Kosevich, Stefano Lepri·Oct 13, 1999SaveLearn
Superconductivity and Topological Numbers in the Hubbard Chain with Bond-Charge InteractionWe determine the quantum phase diagram of the Hubbard chain with electron-hole symmetric correlated hopping at 1/2- and 1/4-filling using geometric concepts and continuum limit field theory. The long…A. A. Aligia, K. Hallberg, C. D. Batista et al.·Oct 12, 1999SaveLearn
Hysteresis in One-Dimensional Anti-Ferromagnetic Random-Field Ising Model at Zero-TemperatureWe analyse hysteresis in a one-dimensional anti-ferromagnetic random field Ising model at zero-temperature. The random field is taken to have a rectangular distribution of width 2 Δ centered about…Prabodh Shukla, Ratnadeep Roy, Emilia Ray·Oct 12, 1999SaveLearn
The Free Energy FormulaThe Onsager formula for the free energy of the two dimensional Ising model with periodic boundary conditions is proved.Yu. M. Zinoviev·Oct 12, 1999SaveLearn
Optimal Fluctuations and Tail States of non-Hermitian OperatorsWe develop a general variational approach to study the statistical properties of the tail states of a wide class of non-Hermitian operators. The utility of the method, which is a refinement of the…A. V. Izyumov, B. D. Simons·Oct 11, 1999SaveLearn
Collective oscillations driven by correlation in the nonlinear optical regimeWe present an analytical and numerical study of the coherent exciton polarization including exciton-exciton correlation. The time evolution after excitation with ultrashort optical pulses can be…Th. Oestreich, L. J. Sham·Oct 11, 1999SaveLearn
First principles study of Li intercalated carbon nanotube ropesWe studied Li intercalated carbon nanotube ropes by using first principles methods. Our results show charge transfer between Li and C and small structural deformation of nanotube due to…Jijun Zhao, Alper Buldum, Jie Han et al.·Oct 9, 1999SaveLearn
Interface dynamics in Hele-Shaw flows with centrifugal forces. Preventing cusp singularities with rotationA class of exact solutions of Hele-Shaw flows without surface tension in a rotating cell is reported. We show that the interplay between injection and rotation modifies drastically the scenario of…F. X. Magdaleno, A. Rocco, J. Casademunt·Oct 8, 1999SaveLearn
On the relation between the anyon and Calogero modelsIn order to achieve a dimensional reduction from dimension two to one not only in phase space but also in configuration space, the lowest Landau level (LLL) projection is not sufficient. One has…Stéphane Ouvry·Oct 8, 1999SaveLearn