Absence of spin gap in the superconducting ladder compound Sr2Ca12Cu24O41Transport and 63Cu-NMR, Knight shift and T1, measurements performed on the two-leg spin ladders of Sr2Ca12Cu24O41 single crystals show a collapse of the gap in ladder spin excitations…H. Mayaffre, P. Auban-Senzier, D. Jérome et al.·Oct 7, 1997SaveLearn
Density matrix renormalization group study of the polaron problem in the Holstein modelWe propose a new density matrix renormalization group (DMRG) approach to study lattices including bosons. The key to the new approach is an exact mapping of a boson site containing 2N states to N…Eric Jeckelmann, Steven R. White·Oct 6, 1997SaveLearn
A Study of the affect of N and B doping on the growth of CVD diamond (100):H 2 X 1 surfacesWe present a study of the effects of Nitrogen and Boron doping on the growth of CVD diamond in the (100) mechanism. These are the first calculations of this type and show that, in accordance with…M. Kaukonen, R. M. Nieminen, P. K. Sitch et al.·Oct 6, 1997SaveLearn
On the integrability of the SU(N) Hubbard modelWe exhibit explicitly the intertwiner operator for the monodromy matrices of the recent proposed SU(N) Hubbard model [5]. This produces a new family of non-additive R-matrices and generalizes an…M. J. Martins·Oct 5, 1997SaveLearn
Beyond the Hubbard-I Solution with a One-Pole Self-Energy at Half-Filling with the Moment Approach: Non-Linear EffectsWe have postulated a single pole for the self-energy, Σ(k,ω), looking for the consequences on the one-particle Green function, G(k,ω) in the Hubbard model. We find that G(k,ω)…J. J. Rodriguez-Nunez, M. A. de Menezes·Oct 4, 1997SaveLearn
The Two - Dimensional Attractive Hubbard Model: Highly Non-Linear Superconductivity With Sum RulesWe use the moment approach of Nolting (exact sum rules) (Z. Physik 255, 25 (1972)) for the attractive Hubbard model in the superconducting phase. Our diagonal and off - diagonal spectral functions…J. J. Rodriguez - Nunez, C. E. Cordeiro, A. Delfino·Oct 4, 1997SaveLearn
Equivalence of the Calogero-Sutherland Model to Free Harmonic OscillatorsA similarity transformation is constructed through which a system of particles interacting with inverse-square two-body and harmonic potentials in one dimension, can be mapped identically, to a set…N. Gurappa, Prasanta. K. Panigrahi·Oct 3, 1997SaveLearn
Exactly integrable family of generalized Hubbard models with twisted Yangian symmetryA strongly correlated electron system with controlled hopping, in the line of the recently proposed generalized Hubbard models as candidates for high Tc-superconductors, is considered. The model…Anjan Kundu·Oct 3, 1997SaveLearn
Spectral Curves of Non-Hermitean HamiltoniansRecent analytical and numerical work have shown that the spectrum of the random non-hermitean Hamiltonian on a ring which models the physics of vortex line pinning in superconductors is one…J. Feinberg, A. Zee·Oct 3, 1997SaveLearn
Instanton in Disordered Peierls SystemsWe study disordered Peierls systems described by the Fluctuating Gap Model. We show that the typical electron states with energies lying deep inside the pseudogap are localized near large disorder…Maxim Mostovoy, Jasper Knoester·Oct 3, 1997SaveLearn
Single-Particle Diffusion-Coefficient on Surfaces with Ehrlich-Schwoebel-BarriersThe diffusion coefficient of single particles in the presence of Ehrlich-Schwoebel barriers (ESB)is considered. An exact expression is given for the diffusion coefficient on linear chains with random…K. Mussawisade, T. Wichmann, K. W. Kehr·Oct 2, 1997SaveLearn
Diffusion process in a deterministically forced flowWe analyze circumstances under which the microscopic dynamics of particles which are driven by a forced, gradient-type flow can be consistently interpreted as a Markovian diffusion process. Special…P. Garbaczewski·Oct 2, 1997SaveLearn
Traveling through potential energy landscapes of disordered materials: the activation-relaxation techniqueA detailed description of the activation-relaxation technique (ART) is presented. This method defines events in the configurational energy landscape of disordered materials, such as a-Si, glasses and…Normand Mousseau, G. T. Barkema·Oct 2, 1997SaveLearn
Thermodynamics of vortex lines in layered superconductorsWe study the dissipative thermodynamics of vortex lines in layered superconductors within a simple string model in the dilute limit of negligible vortex interactions and compute the specific heat…Roberto Iengo, Claudio A. Scrucca·Oct 1, 1997SaveLearn
Quasi-excitations and superconductivity in the t-J model on a ladderWe study the t-J model on a ladder by using slave-fermion-CP1 formalism which is quite useful for study of lightly-doped high-Tc cuprates. By integrating half of spin variables, we obtain a…I. Ichinose, T. Matsui·Oct 1, 1997SaveLearn
Rough droplet model for spherical metal clustersWe study the thermally activated oscillations, or capillary waves, of a neutral metal cluster within the liquid drop model. These deformations correspond to a surface roughness which we characterize…N. Pavloff, C. Schmit·Sep 30, 1997SaveLearn
Theory of Hall Anomaly in the Mixed StateAnalogous to Peierls' arguments for the `anomalous' Hall in metals I demonstrate that the Hall anomaly in the mixed state of superconductors, the sign change of the Hall resistivity, is a…P. Ao·Sep 30, 1997SaveLearn
Localization of Quasiparticles in an NS StructureWe discuss localization of quasiparticles in an extended NS structure in the situation when the reflection from the NS interface is mostly of Andreev kind. The localization of quasiparticle states…A. V. Shytov, P. A. Lee, L. S. Levitov·Sep 30, 1997SaveLearn
Electron Correlation and Jahn-Teller Interaction in Manganese OxidesThe interplay between the electron repulsion U and the Jahn-Teller electron-phonon interation ELR is studied with a large d model for the ferromagnetic state of the manganese oxides. These…Naoto Nagaosa, Shuichi Murakami, Hyun Cheol Lee·Sep 30, 1997SaveLearn
Bridged-assisted electron transfer. Random matrix theory approachWe discuss the effective donor/acceptor coupling for a bridged electron transfer system with a site-diagonal disorder of bridge energies. The average spectral properties of the system are discussed…Ewa Gudowska-Nowak, Gabor Papp, Juergen Brickmann·Sep 30, 1997SaveLearn
Vortex Dynamics, Resistivity Formula, and Fluctuation-dissipation TheoremsWe investigate the problem of forces on moving vortex in a superfluid or superconductor. The main purpose is to locate the source which leads to the contradictory results in the literature. We…X. -M. Zhu, P. Ao·Sep 29, 1997SaveLearn
Vortex lattice transition in D-wave superconductorsMaking use of the extended Ginzburg Landau theory, which includes the fourth order derivative term, we study the vortex state in a magnetic field parallel to the c axis. The vortex core structure…Jun'ichi Shiraishi, Mahito Kohmoto, Kazumi Maki·Sep 29, 1997SaveLearn
Second harmonic generation in SiC polytypesLMTO calculations are presented for the frequency dependent second harmonic generation (SHG) in the polytypes 2H, 4H, 6H, 15R and 3C of SiC. All independent tensor components are calculated. The…Sergey N. Rashkeev, Walter R. L. Lambrecht, Benjamin Segall·Sep 29, 1997SaveLearn
Dynamics of Ordering of Heisenberg Spins with Torque --- Nonconserved Case. IWe study the dynamics of ordering of a nonconserved Heisenberg magnet. The dynamics consists of two parts --- an irreversible dissipation into a heat bath and a reversible precession induced by a…Jayajit Das, Madan Rao·Sep 27, 1997SaveLearn
Phase separation of Bose-Einstein condensatesThe zero-temperature system of two dilute overlapping Bose-Einstein condensates is unstable against long wavelength excitations if the interaction strength between the distinguishable bosons exceeds…Eddy Timmermans·Sep 26, 1997SaveLearn