Numerical analysis of the magnetic-field-tuned superconductor-insulator transition in two dimensionsGround state of the two-dimensional hard-core-boson model subjected to external magnetic field and quenched random chemical potential is studied numerically. In experiments, magnetic-field-tuned…Yoshihiro Nishiyama·Nov 1, 2000SaveLearn
The Exact Solution of 1-D SU(n) Hubbard modelIn this paper we derive out the exact solution of the SU(n) Hubbard model through the coordinate and the algebraic Bethe ansatz methods. The energy spectrum and the Bethe ansatz equations are…Boyu Hou, Dantao Peng, Ruihong Yue·Oct 31, 2000SaveLearn
Does EELS haunt your photoemission measurements?It has been argued in a recent paper by R. Joynt (R. Joynt, Science 284, p 777 (1999)) that in the case of poorly conducting solids the photoemission spectrum close to the Fermi Energy may be…K. Schulte, M. A. James, P. G. Steeneken et al.·Oct 30, 2000SaveLearn
Theory of Ferromagnetism in Diluted Magnetic SemiconductorsCarrier-induced ferromagnetism has been observed in several (III,Mn)V semiconductors. We review the theoretical picture of these ferromagnetic semiconductors that emerges from a model with…Jürgen König, Hsiu-Hau Lin, Allan H. MacDonald·Oct 29, 2000SaveLearn
Eliminating leading corrections to scaling in the 3-dimensional O(N)-symmetric phi4 model: N=3 and 4We study corrections to scaling in the O(3)- and O(4)-symmetric phi4 model on the three-dimensional simple cubic lattice with nearest neighbour interactions. For this purpose, we use Monte Carlo…Martin Hasenbusch·Oct 28, 2000SaveLearn
Muffin Tin Orbitals of Arbitrary OrderWe have derived orbital basis sets from scattering theory. They are expressed as polynomial approximations to the energy dependence of a set of partial waves, in quantized form. The corresponding…O. K. Andersen, T. Saha-Dasgupta·Oct 27, 2000SaveLearn
States without linear counterpart in Bose-Einstein condensatesWe show the existence of stationary solutions of a 1-D Gross-Pitaevskii equation in presence of a multi-well external potential that do not reduce to any of the eigenfunctions of the associated…Roberto D'Agosta, Carlo Presilla·Oct 27, 2000SaveLearn
Negative differential resistance in nanotube devicesCarbon nanotube junctions are predicted to exhibit negative differential resistance, with very high peak-to-valley current ratios even at room temperature. We treat both nanotube p-n junctions and…F. Leonard, J. Tersoff·Oct 27, 2000SaveLearn
Spectral Properties of the k-Body Embedded Gaussian Ensembles of Random MatricesWe consider m spinless Fermions in l > m degenerate single-particle levels interacting via a k-body random interaction with Gaussian probability distribution and k <= m in the limit l to…Luis Benet, Thomas Rupp, Hans A. Weidenmueller·Oct 26, 2000SaveLearn
Non-Universal Behavior of the k-Body Embedded Gaussian Unitary Ensemble of Random MatricesUsing a novel approach, we investigate the shape of the average spectrum and the spectral fluctuations of the k-body embedded unitary ensemble in the limit of large matrix dimension. We identify…Luis Benet, Thomas Rupp, Hans A. Weidenmueller·Oct 26, 2000SaveLearn
Generalized Thermostatistical Description of Intermittency and Non-extensivity in Turbulence and Financial MarketsWe describe a simple and accurate framework for modeling the statistical behavior of both fully developed turbulence and short-term dynamics of financial markets based on the formalism of…F. M. Ramos, C. Rodrigues Neto, R. R. Rosa·Oct 26, 2000SaveLearn
Geometry dominated fluid adsorption on sculptured substratesExperimental methods allow the shape and chemical composition of solid surfaces to be controlled at a mesoscopic level. Exposing such structured substrates to a gas close to coexistence with its…C. Rascon, A. O. Parry·Oct 26, 2000SaveLearn
From favorable atomic configurations to supershell structures: a new interpretation of conductance histogramsTitle: From favorable atomic configurations to supershell structures: a new interpretation of conductance histograms Authors: A. Hasmy (IVIC), E. Medina (IVIC), P.A. Serena (CSIC,IVIC) Comments: 7…A. Hasmy, E. Medina, P. A. Serena·Oct 26, 2000SaveLearn
Statistical Analysis of Native Contact Formation in the Folding of Designed Model ProteinsThe time evolution of the formation probability of native bonds has been studied for designed sequences which fold fast into the native conformation. From this analysis a clear hierarchy of bonds…G. Tiana, R. A. Broglia·Oct 25, 2000SaveLearn
Phase separation in La0.5Ca0.5MnO3 doped with 1% 119Sn detected by Mössbauer spectroscopy1% 119Sn-doped La0.5Ca0.5MnO3 was studied by Mössbauer spectroscopy, magnetic moment and resistivity measurements. The Mössbauer spectra below the charge-ordering temperature are…A. Simopoulos, G. Kallias, E. Devlin et al.·Oct 25, 2000SaveLearn
Diabolical Points in Molecular Magnets with a Four-Fold Easy AxisWe study the points of degeneracy (diabolical points) in magnetic molecules such as Mn12-acetate that have an easy axis of four-fold symmetry. This is done for general magnetic field that need not…Chang-Soo Park, Anupam Garg·Oct 24, 2000SaveLearn
Non-Equilibrium DualityThe dual 'worldline', or 'string', description of adiabatic Ginzburg-Landau field theory near a phase transition in terms of quasi-Brownian strings and loops is well understood. In…R. J. Rivers·Oct 24, 2000SaveLearn
Oscillator Strength of Metallic Carbon NanotubesBased on the tight binding method with hopping integral between the nearest-neighbor atoms, an oscillator strength ∫0∞ ω Re σ(ω) is discussed for armchair and metallic zigzag…H. Yoshioka·Oct 23, 2000SaveLearn
Scattering properties of a cut-circle billiard waveguide with two conical leadsWe examine a two-dimensional electron waveguide with a cut-circle cavity and conical leads. By considering Wigner delay times and the Landauer-Büttiker conductance for this system, we probe the…Kathrin Fuchss, Suhan Ree, L. E. Reichl·Oct 20, 2000SaveLearn
A.model of cation ordering in A(B'xB''1-x)O3 relaxorsWe have shown that the lattice-gas model with four repulsive pair interaction constants (corresponding to the four nearest coordination shells) on a simple cubic lattice is a sufficient model to…S. Lapinskas, E. E. Tornau, A. Rosengren·Oct 20, 2000SaveLearn
Carrier relaxation with LO phonon decay in semiconductor quantum dotsAnalysis of an exactly soluble model of phonons coupled to a carrier in a quantum dot provides a clear illustration of a phonon bottleneck to relaxation. The introduction of three-phonon interactions…S. A. Levetas, M. J. Godfrey, P. Dawson·Oct 20, 2000SaveLearn
Quantum group invariant, nonextensive quantum statistical mechanicsWe study the consequences of introducing quantum group invariance in the formalism of nonextensive quantum statistical mechanics. We find that the corresponding thermodynamical system is equivalent…Marcelo R. Ubriaco·Oct 19, 2000SaveLearn
On Financial Markets TradingStarting from the observation of the real trading activity, we propose a model of a stockmarket simulating all the typical phases taking place in a stock exchange. We show that there is no need of…Lorenzo Matassini, Fabio Franci·Oct 19, 2000SaveLearn
Magnetostriction and magnetoelastic domains in antiferromagnetsThe problem of the observable equilibrium domain structure in pure antiferromagnets (and other thermoelastics) is investigated with the use of continuous elasticity theory. It is shown that…Helen Gomonay, Vadim Loktev·Oct 18, 2000SaveLearn
Exciton-exciton interaction in quantum wells. Optical properties and energy and spin relaxationThe gas of interacting excitons in quantum wells is studied. We obtain the Hamiltonian of this gas by the projection of the electron-hole plasma Hamiltonian to exciton states and an expansion in a…S. Ben-Tabou de-Leon, B. Laikhtman·Oct 18, 2000SaveLearn