Fate of a Bose-Einstein condensate with attractive interactionWe calculate the decay amplitude of a harmonically trapped Bose-Einstein condensate with attractive interaction via the Feynman path integral. We find that when the number of particles is less than a…Masahito Ueda, Kerson Huang·Jul 27, 1998SaveLearn
Kinetic Monte Carlo simulations of the growth of polymer crystalsBased upon kinetic Monte Carlo simulations of crystallization in a simple polymer model we present a new picture of the mechanism by which the thickness of lamellar polymer crystals is constrained to…Jonathan Doye, Daan Frenkel·Jul 27, 1998SaveLearn
Broad Histogram Relation Is ExactThe Broad Histogram is a method designed to calculate the energy degeneracy g(E) from microcanonical averages of certain macroscopic quantities Nup and Ndn. These particular quantities are defined…Paulo Murilo Castro de Oliveira·Jul 27, 1998SaveLearn
Detection of vorticity in Bose-Einstein condensed gases by matter-wave interferenceA phase-slip in the fringes of an interference pattern is an unmistakable characteristic of vorticity. We show dramatic two-dimensional simulations of interference between expanding condensate clouds…Eric L. Bolda, Dan F. Walls·Jul 27, 1998SaveLearn
Structural Transitions and Global Minima of Sodium Chloride ClustersIn recent experiments on sodium chloride clusters structural transitions between nanocrystals with different cuboidal shapes were detected. Here we determine reaction pathways between the low energy…Jonathan Doye, David Wales·Jul 27, 1998SaveLearn
Escape rate of the nanospin system in a magnetic field: the first-order phase transition within quantum regimeWe have investigated the escape rate of the nanospin particle with a magnetic field applied along the easy axis. The model studied here is described by the Hamiltonian $ H = K1 Sz2…Chang Soo Park, Sahng-Kyoon Yoo, D. K. Park et al.·Jul 26, 1998SaveLearn
An Exactly Solvable Model of Generalized Spin LadderA detailed study of an S=12 spin ladder model is given. The ladder consists of plaquettes formed by nearest neighbor rungs with all possible SU(2)-invariant interactions. For properly chosen…S. Albeverio, S. M. Fei, Y. P. Wang·Jul 25, 1998SaveLearn
Electrical Conductivity of Fermi Liquids. II. Quasiparticle TransportWe develop a general theory of Fermi liquids to discuss the Kadowaki-Woods relation A γ2. We derive a formula for the ratio A/γ2 which is expressed as a product of two dimensionless…Takuya Okabe·Jul 25, 1998SaveLearn
Electrical Conductivity of Fermi Liquids. I. Many-body Effect on the Drude WeightOn the basis of the Fermi liquid theory, we investigate the many-body effect on the Drude weight. In a lattice system, the Drude weight D is modified by electron-electron interaction due to Umklapp…Takuya Okabe·Jul 25, 1998SaveLearn
Density-functional study of hydrogen chemisorption on vicinal Si(001) surfacesRelaxed atomic geometries and chemisorption energies have been calculated for the dissociative adsorption of molecular hydrogen on vicinal Si(001) surfaces. We employ density-functional theory,…E. Pehlke, P. Kratzer·Jul 24, 1998SaveLearn
Capture of carriers to screened charged centres and low temperature shallow impurity electric field break down in semiconductorsFree carrier capture by a screened Coulomb potential in semiconductors are considered. It is established that with decreasing screening radius the capture cross section decreases drastically, and it…O. Z. Alekperov·Jul 24, 1998SaveLearn
n-GaAs quality diagnose from shallow impurities photoelectric spectroscopy line shapes dependence on electric fieldIt is established experimentally that the low temperature photoelectric spectra line width of shallow impurities depends not only on charged impurity concentration Ni=2KNA and degree of samples…O. Z. Alekperov·Jul 24, 1998SaveLearn
Multi-connected Momentum Distribution and Fermion CondensationThe structure of the ground state beyond the instability point of the quasiparticle system with Fermi-step momentum distribution is studied within the model of a Fermi liquid with a strong repulsive…M. V. Zverev, M. Baldo·Jul 24, 1998SaveLearn
Ward Identities for Interacting Electronic SystemsA Ward-Takahashi identity, as a consequence of gauge invariance and in a form that relates self-energy to the two-particle Bethe-Salpeter scattering kernel, was first derived by Vollhardt and Wölfle…H. T. Nieh, Ping Sheng, Xiao-Bing Wang·Jul 23, 1998SaveLearn
Avalanche mixing of granular solids in a rotating 2D drum and discrete mappingEvolution of mixing of granular solids in a slowly rotated 2D drum is considered as a discrete mapping. The rotation is around the axis of the upright drum which is filled partially, and the mixing…S. N. Dorogovtsev·Jul 22, 1998SaveLearn
Mesoscopic Physics and the Fundamentals of Quantum MechanicsWe start by reviewing some interesting results in mesoscopic physics illustrating nontrivial insights on Quantum Mechanics. We then review the general principles of dephasing (sometimes called…Yoseph Imry·Jul 22, 1998SaveLearn
Cantori and dynamical localization in the Bunimovich StadiumClassical and quantum properties of the Bunimovich stadium in the diffusive regime are reviewed. In particular, the quantum properties are directly investigated using an approximate quantum map.…Fausto Borgonovi, Paolo Conti, Daniela Rebuzzi et al.·Jul 22, 1998SaveLearn
Simulation of a non-invasive charge detector for quantum cellular automataInformation in a Quantum Cellular Automata architecture is encoded in the polarizazion state of a cell, i.e., in the occupation numbers of the quantum dots of which the cell is made up. Non-invasive…G. Iannaccone, C. Ungarelli, M. Macucci et al.·Jul 22, 1998SaveLearn
Current partition: Nonequilibrium Green's function ApproachWe present a solution to the problem of AC current partition in a multi-probe mesoscopic conductor within the nonequilibrium Green's function formalism. This allows the derivation of dynamic…Baigeng Wang, Jian Wang, Hong Guo·Jul 22, 1998SaveLearn
A Wannier-function-based ab initio Hartree-Fock study of polyethyleneIn the present letter, we report the extension of our Wannier-function-based ab initio Hartree-Fock approach---meant originally for three-dimensional crystalline insulators---to deal with…Alok Shukla, Michael Dolg, Hermann Stoll·Jul 21, 1998SaveLearn
Alternating Spin and Orbital Dimerization in Strong-coupling Two-band ModelsWe study a one-dimensional Hamiltonian consisting of coupled SU(2) spin and orbital degrees of freedom. Using the density matrix renormalization group, we calculate the phase-diagram and the ground…Swapan K. Pati, Rajiv R. P. Singh, Daniel I. Khomskii·Jul 20, 1998SaveLearn
Optical Conductivity in the Copper Oxide MaterialsThe frequency- and temperature-dependent optical conductivity of the copper oxide materials in the underdoped and optimal doped regimes are studied within the t-J model. The conductivity spectrum…Zhongbing Huang, Shiping Feng·Jul 19, 1998SaveLearn
Vortex stabilization in Bose-Einstein condensate of alkali atom gasA quantized vortex in the Bose-Einstein condensation (BEC), which is known to be unstable intrinsically, is demonstrated theoretically to be stabilized by the finite temperature effect. The…Tomoya Isoshima, Kazushige Machida·Jul 17, 1998SaveLearn
Interfacial Structural Changes and Singularities in Non-Planar GeometriesWe consider phase coexistence and criticality in a thin-film Ising magnet with opposing surface fields and non-planar (corrugated) walls. We show that the loss of translational invariance has a…C. Rascon, A. O. Parry·Jul 17, 1998SaveLearn
Transition from Sub-Poissonian to Super-Poissonian Shot Noise in Resonant Quantum WellsWe investigate the transition from sub-Poissonian to super-Poissonian values of the zero-temperature shot noise power of a resonant double barrier of macroscopic cross-section. This transition occurs…Ya. M. Blanter, M. Buttiker·Jul 17, 1998SaveLearn