Intrinsic and extrinsic vortex nucleation mechanisms in the flowWe propose very general vortex nucleation mechanisms analogous to a hydrodynamic instability and calculate associated critical velocity in agreement with experiments. The creation of vortices via…F. V. Kusmartsev·Jun 1, 1996SaveLearn
Effective charge-spin models for quantum dotsIt is shown that at low densities, quantum dots with few electrons may be mapped onto effective charge-spin models for the low-energy eigenstates. This is justified by defining a lattice model based…John H. Jefferson, Wolfgang Häusler·Jun 1, 1996SaveLearn
Grafted Rods: A Tilting Phase TransitionA tilting phase transition is predicted for systems comprising rod like molecules which are irreversibly grafted to a flat surface, so that the non interacting rods are perpendicularly oriented. The…F. Schmid, D. Johannsmann, A. Halperin·May 31, 1996SaveLearn
Hole pairing and phonon dynamics in generalized 2D t-J-Holstein modelsThe formation of hole pairs in the planar t-J model is studied in the presence of independent dynamic vibrations of the in-plane oxygen atoms. In-plane (breathing modes) and out-of-plane…T. Sakai, D. Poilblanc, D. J. Scalapino·May 31, 1996SaveLearn
Spectral Flow, Magnus Force and Mutual Friction via the Geometric Optics Limit of Andreev ReflectionThe notion of spectral flow has given new insight into the motion of vortices in superfluids and superconductors. For a BCS superconductor the spectrum of low energy vortex core states is largely…Michael Stone·May 31, 1996SaveLearn
c axis superfluid response of Copper-Oxide superconductorsA novel interplay between d-wave superconducting order parameter symmetry and the underlying Cu 3d orbital based electronic structure of Copper-Oxides leads to a striking anisotropy in the superfluid…T. Xiang, J. M. Wheatley·May 31, 1996SaveLearn
Finite size effects in Derrida's model multicriticities and limits of generalization for the Zamolodchikov' s C-theoremFinite size effects in the multicriticity point and boundaries between phases are calculated. There are anomalous large finite size effects on the boundary of ferromagnetic phase with paramagnetic or…Y. B. Saakian·May 31, 1996SaveLearn
Theoretical Approach to the Correlations of a Hard-Sphere CrystalWe present the first theoretical approach to the angular-average of the two-body correlation function g(r) for simple solids. It is based on three sum rules for g(r): the…C. Rascon, L. Mederos, G. Navascues·May 31, 1996SaveLearn
d-wave superconductivity near charge instabilitiesWe investigate the symmetry of the superconducting order parameter in the proximity of a phase-separation or of an incommensurate charge-density-wave instability. The attractive effective interaction…A. Perali, C. Castellani, C. Di Castro et al.·May 31, 1996SaveLearn
Voltage-biased quantum wire with impuritiesThe bosonization technique to describe correlated electrons in a one-dimensional quantum wire containing impurities is extended to include an applied voltage source. The external reservoirs are shown…Reinhold Egger, Hermann Grabert·May 31, 1996SaveLearn
Fine structure of excitons in Cu2OThree experimental observations on 1s-excitons in Cu2O are not consistent with the picture of the exciton as a simple hydrogenic bound state: the energies of the 1s-excitons deviate from the…G. M. Kavoulakis, Yia-Chung Chang, Gordon Baym·May 31, 1996SaveLearn
Shadow features and shadow bands in the paramagnetic state of cuprate superconductorsThe conditions for the precursors of antiferromagnetic bands in cuprate superconductors are studied using weak-to-intermediate coupling approach. It is shown that there are, in fact, three different…Y. M. Vilk·May 30, 1996SaveLearn
Persistent currents in interacting electronic systemsPersistent currents in disordered mesoscopic rings threaded by a magnetic flux are calculated using exact diagonalization methods in the one-dimensional (1D) case and self-consistent Hartree-Fock…Georges Bouzerar, Didier Poilblanc·May 30, 1996SaveLearn
Coupling to optical phonons in the one-dimensional t-J model: Effects on superconducting fluctuations and phase separationThe one-dimensional (1D) t-J Holstein model is studied by exact diagonalization of finite rings using a variational approximation for the phonon states. Due to renormalization effects induced by…Roland Fehrenbacher·May 30, 1996SaveLearn
Binary friction tensor for Brownian particles : overcoming spurious finite-size effectsStarting from a careful analysis of the coupled Langevin equations for two interacting Brownian particles, we derive a method for extracting the binary friction tensor from the correlation function…Lydéric Bocquet, Jean-Pierre Hansen, Jaroslaw Piasecki·May 30, 1996SaveLearn
High friction limit of the Kramers equation : the multiple time-scale approachThe purpose of the paper is to give a pedagogical introduction to the multiple time-scale technique, on the example of the high friction limit of the Kramers equation. We begin with a discussion of…Lydéric Bocquet·May 30, 1996SaveLearn
Critical fluctuations in superconductors and the magnetic field penetration depthThe superconducting transition is studied within the one-loop renormalization group in fixed dimension D=3 and at the critical point. A tricritical behavior is found, and for κ> κc, an…Igor F. Herbut, Zlatko Tesanovic·May 30, 1996SaveLearn
Electrostriction of Polar GlassesWe develop a finite temperature theory for the susceptibility and electrostriction of isotropic substances in which permanent electric dipoles are restrained from free rotation by elastic forces. All…J. I. Katz, David R. Nelson·May 29, 1996SaveLearn
The Supersymmetric t-J Model with a BoundaryAn open supersymmetric t-J chain with boundary fields is studied by means of the Bethe Ansatz. Ground state properties for the case of an almost half-filled band and a bulk magnetic field are…Fabian H. L. Essler·May 29, 1996SaveLearn
Microscopic Reversibility and Macroscopic Behavior: Physical Explanations and Mathematical DerivationsThe observed general time-asymmetric behavior of macroscopic systems -- embodied in the second law of thermodynamics -- arises naturally from time-symmetric microscopic laws due to the great…Joel L. Lebowitz·May 29, 1996SaveLearn
Quasiparticle energy dispersion in doped two dimensional quantum antiferromagnetsThe quasiparticle dispersion in the one-hole t-t'-t"-J model is studied. Both the finite-size diagonalization and the self-consistent Born approximation calculations have been performed and…T. Xiang, J. M. Wheatley·May 29, 1996SaveLearn
Force-Extension Relation and Plateau Modulus for Wormlike ChainsWe derive the linear force-extension relation for a wormlike chain of arbitrary stiffness including entropy elasticity, bending and thermodynamic buckling. From this we infer the plateau modulus…Klaus Kroy, Erwin Frey·May 29, 1996SaveLearn
Columnar dimer and plaquette resonating valence bond states of the quantum dimer modelWe study the nature of the ground state of the quantum dimer model proposed by Rokhsar and Kivelson by diagonalizing the Hamiltonian of the model on square lattices of size L× L, where $L≤…P. W. Leung, K. C. Chiu, K. J. Runge·May 29, 1996SaveLearn
Perturbation study on the spin and charge susceptibilities of the two-dimensional Hubbard modelWe investigate the spin and charge susceptibilities of the two-dimensional Hubbard model based upon the perturbative calculation in the strength of correlation U. For U comparable to a bare…Takashi Hotta, Satoshi Fujimoto·May 29, 1996SaveLearn
Undulatory Variation of Antiferromagnetic Strength with Magnetic Field Based on Hubbard Model HamiltonianUsing the Hubbard model Hamiltonian in a mean field level, we examine the variation of antiferromagnetic strength with applied magnetic field. It is demonstrated that minima in the antiferromagnetic…Hyeonjin Doh, Sung-Ho Suck Salk·May 29, 1996SaveLearn