Tensile Strength of Carbon Nanotubes under Realistic Temperature and Strain RateStrain rate and temperature dependence of the tensile strength of single-walled carbon nanotubes has been investigated with molecular dynamics simulations. The tensile failure or yield strain is…Chenyu Wei, Kyeongjae Cho, Deepak Srivastava·Feb 27, 2002SaveLearn
Random-phase approximation study of collective excitations in the Bose-Fermi mixed condensate of alkali-metal gasesWe perform Random Phase Approximation (RPA) study of collective excitations in the bose-fermi mixed degenerate gas of Alkali-metal atoms at T=0. The calculation is done by diagonalization in a model…T. Sogo, T. Miyakawa, T. Suzuki et al.·Feb 26, 2002SaveLearn
Vortex-vortex interactions in toroidally trapped Bose-Einstein condensatesWe analyze the vortex dynamics and vortex-vortex interactions in Bose-Einstein condensates confined in toroidal traps. We show that this particular geometry strongly distorts the vortex dynamics. The…T. Schulte, L. Santos, A. Sanpera et al.·Feb 26, 2002SaveLearn
First-order transition between a small-gap semiconductor and a ferromagnetic metal in the isoelectronic alloys FeSi1-xGexThe contrasting groundstates of isoelectronic and isostructural FeSi and FeGe can be explained within an extended local density approximation scheme (LDA+U) by an appropriate choice of the onsite…V. I. Anisimov, R. Hlubina, M. A. Korotin et al.·Feb 26, 2002SaveLearn
History-dependent Maximum Static Friction and Rectification of a System with a Few Particles in a Periodic FieldHistory-dependent maximum static friction is investigated using simple models with two and three particles in one-dimensional periodic potentials. In some situations, these systems possess two values…A. Awazu·Feb 26, 2002SaveLearn
Contrast Interferometry Using Bose-Einstein Condensates to Measure h/m and the Fine Structure ConstantThe kinetic energy of an atom recoiling due to absorption of a photon was measured as a frequency using an interferometric technique called ``contrast interferometry''. Optical standing wave…S. Gupta, K. Dieckmann, Z. Hadzibabic et al.·Feb 25, 2002SaveLearn
On Kelvin-Helmholtz instability in superfluidsThe Kelvin-Helmholtz instability in superfluids is discussed, based on the first experimental observation of such instability at the interface between superfluid 3He-A and superfluid 3He-B…G. E. Volovik·Feb 25, 2002SaveLearn
Thixotropy in macroscopic suspensions of spheresAn experimental study of the viscosity of a macroscopic suspension, i.e. a suspension for which Brownian motion can be neglected, under steady shear is presented. The suspension is prepared with a…C. Voeltz, M. Nitschke, L. Heymann et al.·Feb 25, 2002SaveLearn
Magnetic field driven metal-insulator phase transition in planar systemsA theory of the magnetic field driven (semi-)metal-insulator phase transition is developed for planar systems with a low density of carriers and a linear (i.e., relativistic like) dispersion relation…E. V. Gorbar, V. P. Gusynin, V. A. Miransky et al.·Feb 24, 2002SaveLearn
Phase Diagram of the Extended Hubbard Model with Pair Hopping InteractionA one-dimensional model of interacting electrons with on-site U, nearest-neighbor V, and pair-hopping interaction W is studied at half-filling using the continuum limit field theory approach.…G. I. Japaridze, Sujit Sarkar·Feb 24, 2002SaveLearn
Sparse random matrices: the eigenvalue spectrum revisitedWe revisit the derivation of the density of states of sparse random matrices. We derive a recursion relation that allows one to compute the spectrum of the matrix of incidence for finite trees that…Guilhem Semerjian, Leticia F. Cugliandolo·Feb 22, 2002SaveLearn
Scaling of nano-Schottky-diodesA generally applicable model is presented to describe the potential barrier shape in ultra small Schottky diodes. It is shown that for diodes smaller than a characteristic length lc (associated…G. D. J. Smit, S. Rogge, T. M. Klapwijk·Feb 22, 2002SaveLearn
Magnetic properties of SO(5) superconductivityThe distinction between type I and type II superconductivity is re-examined in the context of the SO(5) model recently put forth by Zhang. Whereas in conventional superconductivity only one parameter…M. Juneau, R. MacKenzie, M. -A. Vachon·Feb 22, 2002SaveLearn
Variational Perturbation Theory for Markov ProcessesWe develop a convergent variational perturbation theory for conditional probability densities of Markov processes. The power of the theory is illustrated by applying it to the diffusion of a particle…Hagen Kleinert, Axel Pelster, Mihai V. Putz·Feb 21, 2002SaveLearn
Optical RKKY Interaction between Charged Semiconductor Quantum DotsWe show how a spin interaction between electrons localized in neighboring quantum dots can be induced and controlled optically. The coupling is generated via virtual excitation of delocalized…C. Piermarocchi, Pochung Chen, L. J. Sham et al.·Feb 20, 2002SaveLearn
Tunable Quantum Tunneling of Magnetic Domain WallsMagnetic domain wall tunneling is observed in the disordered Ising ferromagnet LiHo0.44Y0.56F4. The tunneling can be tuned by applying a magnetic field transverse to the Ising axis, and is…J. Brooke, T. F. Rosenbaum, G. Aeppli·Feb 20, 2002SaveLearn
Topology of the ground state of two interacting Bose-Einstein condensatesWe investigate the spatial patterns of the ground state of two interacting Bose-Einstein condensates. We consider the general case of two different atomic species (with different mass and in…Francesco Riboli, Michele Modugno·Feb 20, 2002SaveLearn
Quantization of adiabatic pumped charge in the presence of superconducting leadWe investigate the parametric electron pumping of a double barrier structure in the presence of a superconducting lead. The parametric pumping is facilitated by cyclic variation of the barrier…Jian Wang, Baigeng Wang·Feb 20, 2002SaveLearn
Nature of the spin-singlet ground state in CaCuGe2O6We investigate by means of ab initio electronic structure analysis and Quantum Monte Carlo calculations the scenario where longer-ranged magnetic interactions dominate over short-ranged interactions…Roser Valenti, T. Saha-Dasgupta, Claudius Gros·Feb 19, 2002SaveLearn
Calculation of the energy spectrum of a two-electron spherical quantum dotWe study the energy spectrum of the two-electron spherical parabolic quantum dot using the exact Schroedinger, the Hartree-Fock, and the Kohn-Sham equations. The results obtained by applying the…Ramiro Pino, Victor M. Villalba·Feb 19, 2002SaveLearn
Generating vortex rings in Bose-Einstein condensates in the line-source approximationWe present a numerical method for generating vortex rings in Bose-Einstein condensates confined in axially symmetric traps. The vortex ring is generated using the line-source approximation for the…M. Guilleumas, D. M. Jezek, R. Mayol et al.·Feb 19, 2002SaveLearn
Option Pricing from Path Integral for Non-Gaussian Fluctuations. Natural Martingale and Application to Truncated Lévy DistributionsWithin a path integral formalism for non-Gaussian price fluctuations we set up a simple stochastic calculus and derive a natural martingale for option pricing from the wealth balance of options,…Hagen Kleinert·Feb 19, 2002SaveLearn
Quantum-fluctuation-induced collisions and subsequent excitation gap of an elastic string between wallsAn elastic string embedded between rigid walls is simulated by means of the density-matrix renormalization group. The string collides against the walls owing to the quantum-mechanical zero-point…Yoshihiro Nishiyama·Feb 18, 2002SaveLearn
A theory of viscoelastic nematodynamicsA nonlinear viscoelastic theory of nematodynamic type is developed for nematic liquid crystalline (LC) semi-flexible polymers. A measure of transient elastic strain due to the change in length of…A. I. Leonov, V. S. Volkov·Feb 16, 2002SaveLearn
Combinatorial interpretation of Haldane-Wu fractional exclusion statisticsAssuming that the maximal allowed number of identical particles in state is an integer parameter, q, we derive the statistical weight and analyze the associated equation which defines the statistical…A. K. Aringazin, M. I. Mazhitov·Feb 16, 2002SaveLearn