The Cumulant Expansion for the Anderson Lattice with Finite U: The Completeness Problem``Completeness'' (i.e. probability conservation) is not usually satisfied in the cumulant expansion of the Anderson lattice when a reduced state space is employed for U ∞ . To…M. E. Foglio, M. S. Figueira·Feb 27, 1998SaveLearn
Fluctuation-induced phase in CsCuCl3 in transverse magnetic field: TheoryCsCuCl3 is a quantum triangular antiferromagnet, ferromagnetically stacked, with an incommensurate (IC) structure due to a Dzyaloshinskii-Moriya interaction. Because of the classical degeneracy…A. E. Jacobs, Tetsuro Nikuni·Feb 27, 1998SaveLearn
Statistics of S-matrix poles for chaotic systems with broken time reversal invariance: a conjectureIn the framework of a random matrix description of chaotic quantum scattering the positions of S-matrix poles are given by complex eigenvalues Zi of an effective non-Hermitian random-matrix…Yan V. Fyodorov, Mikhail Titov, H. -J. Sommers·Feb 27, 1998SaveLearn
Fokker-Planck Equations for Nucleation Processes RevisitedWe present a new approach to analyze homogeneous nucleation based on non-equilibrium thermodynamics. The starting point is the formulation of a Gibbs equation for the variations of the entropy of the…D. Reguera Lopez, J. M. Rubi, A. Perez-Madrid·Feb 27, 1998SaveLearn
Correlation functions in the Calogero-Sutherland model with open boundariesCalogero-Sutherland models of type BCN are known to be relevant to the physics of one-dimensional quantum impurity effects. Here we represent certain correlation functions of these models in terms…Holger Frahm, Sergey I. Matveenko·Feb 26, 1998SaveLearn
Electron renormalization of sound interaction with two-level systems in superconducting metglassesThe crossing of temperature dependences of the sound velocity in normal and superconducting state of metallic glasses points out unambiguously the renormalization of the intensity of sound…E. V. Bezuglyi, A. L. Gaiduk, V. D. Fil et al.·Feb 26, 1998SaveLearn
Resistivity due to low-symmetrical defects in metalsThe impurity resistivity, also known as the residual resistivity, is calculated ab initio using multiple-scattering theory. The mean-free path is calculated by solving the Boltzmann equation…J. P. Dekker, A. Lodder, J. van Ek·Feb 26, 1998SaveLearn
Identification of Non-unitary triplet pairing in a heavy Fermion superconductor UPt3A NMR experiment recently done by Tou et al. on a heavy Fermion superconductor UPt3 is interpreted in terms of a non-unitary spin-triplet pairing state which we have been advocating. The proposed…Kazushige Machida, Tetsuo Ohmi·Feb 26, 1998SaveLearn
Instability of charge ordered states in doped antiferromagnetsWe analyze the induced interactions between localized holes in weakly-doped Heisenberg antiferromagnets due to the modification of the quantum zero point spin wave energy; i.e. the analogue of the…Leonid P. Pryadko, Steven Kivelson, Daniel W. Hone·Feb 26, 1998SaveLearn
Transition from Poisson to gaussian unitary statistics: The two-point correlation functionWe consider the Rosenzweig-Porter model of random matrix which interpolates between Poisson and gaussian unitary statistics and compute exactly the two-point correlation function. Asymptotic formulas…H. Kunz, B. Shapiro·Feb 25, 1998SaveLearn
Destruction of Strong Critical Spin Fluctuations by Doping in the 2D Hubbard ModelWe present the doping dependence of the spectral functions, density of states and low frequency behavior of the self-energy for the 2D Hubbard model on the basis of our recently developed theory for…Bumsoo Kyung·Feb 25, 1998SaveLearn
Electromagnetic forces in photonic crystalsWe develop a general methodology for numerical computations of electromagnetic (EM) fields and forces in matter, based on solving the macroscopic Maxwell's equations in real space and adopting…M. I. Antonoyiannakis, J. B. Pendry·Feb 24, 1998SaveLearn
Band Kondo Effect in the Doped 2D Hubbard ModelWe present strong numerical evidence for the band Kondo effect in the doped 2D Hubbard model by showing the systematic change of the density of states, imaginary part of the self-energy, effective…Bumsoo Kyung·Feb 24, 1998SaveLearn
Excitation spectrum and instability of a two-species Bose-Einstein condensateWe numerically calculate the density profile and excitation spectrum of a two-species Bose-Einstein condensate for the parameters of recent experiments. We find that the ground state density profile…D. Gordon, C. M. Savage·Feb 24, 1998SaveLearn
DMRG Calculations of the Low-lying Excitations and Nonlinear Optical Properties of poly(para-phenylene)The two state molecular orbital (2-MO) model of the phenyl based semiconductors is used to calculate the low-lying spectra of the Ag and Bu states of poly(para-phenylene) (PPP). The model parameters…W. Barford, R. J. Bursill, M. Yu. Lavrentiev·Feb 23, 1998SaveLearn
Distributions of gaps and end-to-end correlations in random transverse-field Ising spin chainsA previously introduced real space renormalization-group treatment of the random transverse-field Ising spin chain is extended to provide detailed information on the distribution of the energy gap…Daniel S. Fisher, A. P. Young·Feb 23, 1998SaveLearn
Quantum Field Theory of Vortices in Superfluid FilmsA quantum field theory, consisting of the effective action of sound waves linearly coupled to a Chern-Simons term, is proposed to describe the dynamics of vortices in a superfluid film at the…Joerg P. Kottmann, Adriaan M. J. Schakel·Feb 23, 1998SaveLearn
The many-Electron Problem in Novel Low-Dimensional MaterialsThis work deals with the one-dimensional Hubbard model. It has seven chapters: 1. Introduction; 2. The Hubbard Model; 3. Algebraic Representation for the Hilbert Space of the 1D Hubbard Model; 4.…N. M. R. Peres·Feb 23, 1998SaveLearn
Density-Induced Breaking of Pairs in the Attractive Hubbard ModelA conserving T-matrix approximation is applied to the two-dimensional attractive Hubbard model in the low-density regime. A set of self-consistent equations is solved in the real-frequency domain to…Bumsoo Kyung, E. G. Klepfish, P. E. Kornilovitch·Feb 23, 1998SaveLearn
Scattering of He-3 Atoms from He-4 SurfacesWe develop a first principles, microscopic theory of impurity atom scattering from inhomogeneous quantum liquids such as adsorbed films, slabs, or clusters of He-4. The theory is built upon a…E. Krotscheck, R. Zillich·Feb 21, 1998SaveLearn
The Relevant Operators for the Hubbard Hamiltonian with a magnetic field termThe Hubbard Hamiltonian and its variants/generalizations continue to dominate the theoretical modelling of important problems such as high temperature superconductivity. In this note we identify the…S. Alam, M. Nasir Khan, Jauhar Ali·Feb 21, 1998SaveLearn
Phase diagram of the one-dimensional Holstein model of spinless fermionsThe one-dimensional Holstein model of spinless fermions interacting with dispersionless phonons is studied using a new variant of the density matrix renormalisation group. By examining various…R. J. Bursill, R. H. McKenzie, C. J. Hamer·Feb 20, 1998SaveLearn
Identification of excitons in conjugated polymers: a density matrix renormalisation group studyThis work addresses the question of whether low-lying excitations in conjugated polymers are comprised of free charge-carriers or excitons. States are characterised as bound or unbound according to…M. Boman, R. J. Bursill·Feb 20, 1998SaveLearn
Density of kinks just after a quench in an overdamped systemA quench in an overdamped one dimensional ϕ4 model is studied by analytical and numerical methods. For an infinite system or a finite system with free boundary conditions, the density of kinks…Jacek Dziarmaga·Feb 19, 1998SaveLearn
Low temperature phase diagram and critical behaviour of the four-state chiral clock modelThe low temperature behaviour of the four-state chiral clock (CC4) model is reexamined using a systematic low temperature series expansion of the free energy. Previously obtained results for the…M. Pleimling, B. Neubert, R. Siems·Feb 19, 1998SaveLearn