An Exactly Solvable Kondo Problem for Interacting One-Dimensional FermionsThe single impurity Kondo problem in the one-dimensional δ-potential Fermi gas is exactly solved for two sets of special coupling constants via Bethe ansatz. It is found that ferromagnetic Kondo…Yupeng Wang, Johannes Voit·Sep 18, 1996SaveLearn
Fluid Vesicles in Shear FlowThe shape dynamics of fluid vesicles is governed by the coupling of the flow within the two-dimensional membrane to the hydrodynamics of the surrounding bulk fluid. We present a numerical scheme…Martin Kraus, Wolfgang Wintz, Udo Seifert et al.·Sep 18, 1996SaveLearn
Stability of vortex lines in liquid 3He-4He mixtures at zero temperatureAt low temperatures and 3He concentrations below 6.6 %, there is experimental evidence about the existence in liquid helium mixtures, of stable vortices with 3He-rich cores. When the system is either…D. Jezek, M. Guilleumas, M. Pi et al.·Sep 18, 1996SaveLearn
Properties of Fluctuations in Two Coupled Chains of Luttinger LiquidsTwo chains of Luttinger liquids coupled by both interchain hopping and interchain interaction are investigated. A degeneracy of two kinds of dominant states with in phase and out of phase ordering in…Hideo Yoshioka, Yoshikazu Suzumura·Sep 18, 1996SaveLearn
Frozen Disorder in a Driven SystemWe investigate the effects of quenched disorder on the universal properties of a randomly driven Ising lattice gas. The Hamiltonian fixed point of the pure system becomes unstable in the presence of…B. Schmittmann, K. E. Bassler·Sep 17, 1996SaveLearn
Self-consistent Treatment of Crystal-Electric-Field-Levels in the Anderson LatticeWe consider an Anderson lattice model with a spin 1/2 degenerated conduction electron band and localized ionic CEF-levels, classified according to the irreducible representation of the point group of…F. B. Anders, D. L. Cox·Sep 17, 1996SaveLearn
Low-Lying Electronic Excitations and Nonlinear Optic Properties of Polymers via Symmetrized Density Matrix Renormalization Group MethodA symmetrized Density Matrix Renormalization Group procedure together with the correction vector approach is shown to be highly accurate for obtaining dynamic linear and third order polarizabilities…S. Ramasesha, Swapan K. Pati, H. R. Krishnamurthy et al.·Sep 17, 1996SaveLearn
Phase ordering of the O(2) model in the post-gaussian approximationThe gaussian closure approximation previously used to study the growth kinetics of the non-conserved O(n) model is shown to be the zeroth-order approximation in a well-defined sequence of…Robert A. Wickham, Gene F. Mazenko·Sep 17, 1996SaveLearn
Strong coupling phases of the t-t' Hubbard modelWe study the strong coupling regime of the t-t' Hubbard model,filled up to the level of the van Hove singularities, by means of an exact diagonalization approach. We characterize the different…J. Gonzalez, J. V. Alvarez·Sep 17, 1996SaveLearn
On the gap structure of UPt3: phases A and BWe have used thermal conduction and transverse sound attenuation to probe the anisotropy of the gap structure in two superconducting phases of UPt3. For the low-temperature phase B, transverse…Louis Taillefer, Brett Ellman, Benoit Lussier et al.·Sep 17, 1996SaveLearn
Stokes shift in quantum wells: trapping versus thermalizationLow temperature photoluminescence and photoluminescence excitation measurements have been performed in a set of InGaAs/GaAs samples with different indium molar fraction, well width, growth conditions…A. Polimeni, A. Patanè, M. Grassi Alessi et al.·Sep 17, 1996SaveLearn
Renormalization-group study of a magnetic impurity in a Luttinger liquidA generalized Anderson model for a magnetic impurity in an interacting one-dimensional electron gas is studied via a mapping onto a classical Coulomb gas. For weak potential scattering, the…Avraham Schiller, Kevin Ingersent·Sep 17, 1996SaveLearn
The orbital and charge ordering in Pr1-xCaxMnO3 (x=0 and 0.5) from the ab initio calculationsThe electronic structure of the doped manganites Pr1-xCaxMnO3 was calculated by the LSDA+U method which takes into account the local Coulomb interaction between d-electrons of transition…V. I. Anisimov, I. S. Elfimov, M. A. Korotin et al.·Sep 17, 1996SaveLearn
Random Matrix Theory and Classical Statistical Mechanics. I. Vertex ModelsA connection between integrability properties and general statistical properties of the spectra of symmetric transfer matrices of the asymmetric eight-vertex model is studied using random matrix…H. Meyer, J. -C. Anglès d'Auriac, J. -M. Maillard·Sep 17, 1996SaveLearn
Quantum and Thermal Depinning of a String from a Linear DefectThe problem of a massive elastic string depinning from a linear defect under the action of a small driving force is considered. To exponential accuracy the decay rate is calculated with the help of…Mikhail A. Skvortsov·Sep 17, 1996SaveLearn
Transverse optical plasmons in layered superconductorsWe discuss the possible existance of transverse optical plasma modes in superlattices consisting of Josephson coupled superconducting layers. These modes appear as resonances in the current-current…D. van der Marel, A. Tsvetkov·Sep 17, 1996SaveLearn
Spin-density wave versus superconducting fluctuations for quasi-one-dimensional electrons in two chains of Tomonaga-Luttinger liquidsWe study possible states at low temperatures by applying the renormalization-group method to two chains of Tomonaga-Luttinger liquids with both repulsive intrachain interactions and interchain…Hideo Yoshioka, Yoshikazu Suzumura·Sep 17, 1996SaveLearn
Metallic spin glassesRecent work on the zero temperature phases and phase transitions of strongly random electronic system is reviewed. The transition between the spin glass and quantum paramagnet is examined, for both…Subir Sachdev, N. Read·Sep 17, 1996SaveLearn
Phase Separation in the Two-Dimensional Hubbard ModelBy making use of known exact results and symmetry properties for the one-band Hubbard model, we show in a somewhat exact manner that there is no phase separation on a square lattice at arbitrary…Gang Su·Sep 17, 1996SaveLearn
Radial distribution function of semiflexible polymersWe calculate the distribution function of the end--to--end distance of a semiflexible polymer with large bending rigidity. This quantity is directly observable in experiments on single semiflexible…Jan Wilhelm, Erwin Frey·Sep 17, 1996SaveLearn
Dynamical Renormalization Group Study of a Conserved Surface Growth with Anti-Diffusive and Nonlinear CurrentsBased on dynamical renormalization group (RG) calculations to the one-loop order, the surface growth described by a nonlinear stochastic conserved growth equation, ∂ h ∂ t = …Youngkyun Jung, In-mook Kim, Yup Kim·Sep 17, 1996SaveLearn
Topological Dislocations and Mixed State of Charge Density WavesWe discuss the possibility of the ``mixed state'' in incommensurate charge density waves with three-dimensional order. It is shown that the mixed state can be created by applying an electric…Masahiko Hayashi, Hideo Yoshioka·Sep 17, 1996SaveLearn
A topological characterization of delocalization in a spin-orbit coupling systemWe show that wavefunctions in a two-dimensional (2D) electron system with spin-orbit coupling can be characterized by a topological quantity--the Chern integer due to the existence of the intrinsic…D. N. Sheng, Z. Y. Weng·Sep 17, 1996SaveLearn
Non Fermi Liquid Dynamics of the Two-Channel Kondo LatticeThe paramagnetic phase of the two-channel Kondo lattice model is examined with a Quantum Monte Carlo simulation in the limit of infinite dimensions. We find non-Fermi-liquid behavior at low…M. Jarrell, Hanbin Pang, D. L. Cox et al.·Sep 17, 1996SaveLearn
Dynamical Vortices in Superfluid FilmsThe coupling of vortices to phonons in a superfluid is a gauge coupling dictated by topology. The density and current response to a moving vortex are computed and contrasted with the standard…D. P. Arovas, J. A. Freire·Sep 16, 1996SaveLearn