Numerical analysis of the dissipative two-state system with the density-matrix Hilbert-space-reduction algorithmGround state of the dissipative two-state system is investigated by means of the Lanczos diagonalization method. We adopted the Hilbert-space-reduction scheme proposed by Zhang, Jeckelmann and White…Yoshihiro Nishiyama·Apr 19, 1999SaveLearn
Spin-Charge Binding Mechanism for Superconductivity in CupratesA spin-charge recombination route to superconductivity, proposed earlier (1992)], is examined using the Schwinger boson representation of the t-J model. The representation is known to work well at…Sanjoy K. Sarker·Apr 19, 1999SaveLearn
Orientational phase transitions in anisotropic rare-earth magnets at low temperaturesOrientational phase transitions are investigated within the Heisenberg model with single-site anisotropy. The temperature dependence of the cone angle is calculated within the spin-wave theory. The…V. Yu. Irkhin, A. A. Katanin·Apr 18, 1999SaveLearn
Bcc 4He as a Coherent Quantum SolidIn this work we investigate implications of the quantum nature of bcc 4% He. We show that it is a unique solid phase with both a lattice structure and an Off-Diagonal Long Range Order of…Nir Gov·Apr 18, 1999SaveLearn
The sublattice magnetizations of the spin-s quantum Heisenberg antiferromagnetsWe study the spin-s quantum Heisenberg antiferromagnetic models in a magnon theory free of any unphysical magnon state. Because the unphysical magnon states are completely removed in the magnon…Bang-Gui Liu·Apr 17, 1999SaveLearn
Low energy transition in spectral statistics of 2D interactingfermionsWe study the level spacing statistics P(s) and eigenstate properties of spinless fermions with Coulomb interaction on a two dimensional lattice at constant filling factor and various disorder…Pil Hun Song, Dima L. Shepelyansky·Apr 16, 1999SaveLearn
Specific heat and magnetic order in LaMnO3+δMagnetic and specific-heat measurements are performed in three different samples of LaMnO3+δ, with δ=0.11, 0.15 and 0.26, presenting important disorder effects, such as carrier localization, due…L. Ghivelder, I. Abrego Castillo, M. A. Gusmao et al.·Apr 16, 1999SaveLearn
Fractional statisticWe improve Haldane's formula which gives the number of configurations for N particles on d states in a fractional statistic defined by the coupling g=l/m. Although nothing is changed in the…M. C. Bergère·Apr 16, 1999SaveLearn
Electronic states of metallic and semiconducting carbon nanotubes with bond and site disorderDisorder effects on the density of states in carbon nanotubes are analyzed by a tight binding model with Gaussian bond or site disorder. Metallic armchair and semiconducting zigzag nanotubes are…Kikuo Harigaya·Apr 16, 1999SaveLearn
Microscopic Simulation of Reaction-Diffusion Processes and Applications to Population Biology and Product MarketingWe simulate reaction-diffusion processes with discrete fields. We use a novel algorithm to simulate different autocatalytic processes with trace densities. Anderson localization with a diffusive…Eldad Bettelheim, Benny Lehmann·Apr 14, 1999SaveLearn
Anomalous Transient Current in Nonuniform SemiconductorsNonequilibrium processes in semiconductors are considered with highly nonuniform initial densities of charge carriers. It is shown that there exist such distributions of charge densities under which…V. I. Yukalov, E. P. Yukalova, M. R. Singh·Apr 14, 1999SaveLearn
QHE of Bilayer Systems in the Presence of Tunneling -- ν=1/q case --Transport properties of bilayer quantum Hall systems at ν=1/q, where q is an odd integer, are investigated. The edge theory is used for the investigation, since tunneling between the two layers…Kentaro Nomura, Daijiro Yoshioka·Apr 14, 1999SaveLearn
Irreversible Magnetization of Pin-Free Type II SuperconductorsThe magnetization curve of a type II superconductor in general is hysteretic even when the vortices exhibit no volume or surface pinning. This geometric irreversibility, caused by an edge barrier for…Ernst Helmut Brandt·Apr 14, 1999SaveLearn
cond-mat/9806011This paper has been withdrawn by the authors.Brahim Elattari, Rochus Klesse·Apr 14, 1999SaveLearn
Minimal Potentials with Very Many MinimaWe demonstrate, by construction, that simple renormalizable matrix potentials with SN, as opposed to O(N), symmetry can exhibit an exponentially large number of inequivalent deep local minima.Marin Soljacic, Frank Wilczek·Apr 13, 1999SaveLearn
Exact solution for two interacting electrons on artificial atoms and molecules in solidsWe present a general scheme for finding the exact eigenstates of two electrons, with on-site repulsive potentials Ui, on I impurities in a macroscopic crystal. The model describes impurities in…A. Aharony, O. Entin-Wohlman, Y. Imry·Apr 13, 1999SaveLearn
Step fluctuations and random walksThe probability distribution p(l) of an atom to return to a step at distance l from the detachment site, with a random walk in between, is exactly enumerated. In particular, we study the dependence…M. Bisani, W. Selke·Apr 13, 1999SaveLearn
Functional Renormalization Description of the Roughening TransitionWe reconsider the problem of the static thermal roughening of an elastic manifold at the critical dimension d=2 in a periodic potential, using a perturbative Functional Renormalization Group…Anusha Hazareesing, Jean-Philippe Bouchaud·Apr 13, 1999SaveLearn
Josephson tunneling between weakly interacting Bose-Einstein condensatesBased on a tunneling Hamiltonian description, we calculate the Josephson, normal and interference currents between two Bose-Einstein condensates described by the Bogoliubov theory. The dominant…F. Meier, W. Zwerger·Apr 12, 1999SaveLearn
Ratchet potential for fluxons in Josephson-Junction arraysWe propose a simple configuration of a one-dimensional parallel array of Josephson junctions in which the pinning potential for trapped fluxons lacks inversion symmetry (ratchet potential). This…Fernando Falo, Pedro J. Martinez, Juan J. Mazo et al.·Apr 12, 1999SaveLearn
Projected SO(5) ModelsWe construct a class of projected SO(5) models where the Gutzwiller constraint of no-double-occupancy is implemented exactly. We introduce the concept of projected SO(5) symmetry where all static…Shou-Cheng Zhang, Jiang-Ping Hu, Enrico Arrigoni et al.·Apr 10, 1999SaveLearn
Phonon-induced spin relaxation of conduction electrons in aluminumSpin-flip Eliashberg function αS2F and temperature-dependent spin relaxation time T1(T) are calculated for aluminum using realistic pseudopotentials. The spin-flip electron-phonon coupling…Jaroslav Fabian, S. Das Sarma·Apr 9, 1999SaveLearn
An exactly solvable many-body problem in one dimensionFor N impenetrable particles in one dimension where only the nearest and next-to-nearest neighbours interact, we obtain the complete spectrum both on a line and on a circle. Further, we establish a…Sudhir R. Jain, Avinash Khare·Apr 9, 1999SaveLearn
Timesaving Double-Grid Method for Real-Space Electronic-Structure CalculationsWe present a simple and efficient technique in ab initio electronic-structure calculation utilizing real-space double-grid with a high density of grid points in the vicinity of nuclei. This technique…Tomoya Ono, Kikuji Hirose·Apr 8, 1999SaveLearn
Travelling waves in a drifting flux latticeStarting from the time-dependent Ginzburg-Landau (TDGL) equations for a type II superconductor, we derive the equations of motion for the displacement field of a moving vortex lattice without inertia…R. Aditi Simha, Sriram Ramaswamy·Apr 8, 1999SaveLearn