Triangular AntiferromagnetsIn this article we review the effects of magnetic frustation in the stacked triangular lattice. Frustration increases the degeneracy of the ground state, giving rise to different physics. In…M. F. Collins, O. A. Petrenko·Jun 15, 1997SaveLearn
Baryon Asymmetry of Universe: View from Superfluid 3HeThe origin of the excess of matter over antimatter in our Universe remains one of the fundamental problems. The dynamical baryogenesis in the process of the broken symmetry electroweak transition in…G. E. Volovik·Jun 14, 1997SaveLearn
Aspects of Dielectric Breakdown in a Model for Disordered Nonlinear CompositesWe study dielectric breakdown in a semi-classical bond percolation model for nonlinear composite materials introduced by us and the related breakdown exponent near the percolation threshold in two…Abhijit Kar Gupta, Asok K. Sen·Jun 14, 1997SaveLearn
Integrable su(3) spin chain combining different representationsThe general expression for the local matrix t(θ) of a quantum chain with the site space in any representation of su(3) is obtained. This is made by generalizing t(θ) from the fundamental…J. Abad, M. Ríos·Jun 13, 1997SaveLearn
Electrical Conduction in Nonlinear CompositesStudy of various interesting features related to the nonlinear electrical response in composite materials through a model bond percolative system.Abhijit Kar Gupta, Asok K. Sen·Jun 12, 1997SaveLearn
Comment on `Formation of a Dodecagonal Quasicrystalline Phase in a Simple Monatomic Liquid'In a recent paper M. Dzugutov, Phys. Rev. Lett. 70 2924 (1993), describes a molecular dynamics cooling simulation where he obtained a large monatomic dodecagonal quasicrystal from a melt. The…J. Roth·Jun 12, 1997SaveLearn
Random tiling quasicrystals in three dimensionsThree-dimensional icosahedral random tilings with rhombohedral cells are studied in the semi-entropic model. We introduce a global energy measure defined by the variance of the quasilattice points in…W. Ebinger, J. Roth, H. -R. Trebin·Jun 12, 1997SaveLearn
Random Tiling Transition in Three DimensionsThree-dimensional icosahedral random tilings are studied in the semi-entropic model. We introduce a global energy measure defined by the variance of the quasilattice points in orthogonal space. The…W. Ebinger, J. Roth, H. -R. Trebin·Jun 12, 1997SaveLearn
Icosahedral coincidence rotationsThe coincidence problem for three-dimensional discrete structures with icosahedral symmetry is reinvestigated. We present a parametric description of the coincidence rotations based on special…Johannes Roth, Reinhard Lück·Jun 12, 1997SaveLearn
Relaxation process in a regime of quantum chaosWe show that the quantum relaxation process in a classically chaotic open dynamical system is characterized by a quantum relaxation time scale tq. This scale is much shorter than the Heisenberg time…Giulio Casati, Giulio Maspero, Dima L. Shepelyansky·Jun 11, 1997SaveLearn
Generalized CP1 model from t1-t2-J modelA long-wavelength, low-frequency effective theory is obtained from t1-t2-J model. The action is written in terms of two-component bose spinor fields (CP1 fields) and two spinless Fermi fields.…Naoum Karchev·Jun 11, 1997SaveLearn
Dualities in Spin LaddersWe introduce a set of discrete modular transformations T,U and S in order to study the relationships between the different phases of the Heisenberg ladders obtained with all…German Sierra, Miguel A. Martin-Delgado·Jun 11, 1997SaveLearn
Interface dynamics at the depinning transitionWe study the local scaling properties of driven interfaces in disordered media modeled by the Edwards-Wilkinson equation with quenched noise. We find that, due to the super-rough character of the…Juan M. Lopez, Miguel A. Rodriguez·Jun 11, 1997SaveLearn
Pair Correlations in Superfluid Helium 3In 1996 Lee, Osheroff and Richardson received the Nobel Prize for their 1971 discovery of superfluid helium 3 -- a discovery which opened the door to the most fascinating system known in condensed…D. Vollhardt·Jun 11, 1997SaveLearn
Simultaneous Brownian Motion of N Particles in a Temperature GradientA system of N Brownian particles suspended in a nonuniform heat bath is treated as a thermodynamic system whith internal degrees of freedom, in this case their velocities and coordinates. Applying…J. M. Rubí, P. Mazur·Jun 9, 1997SaveLearn
Tight-Binding study of the electronic and magnetic properties of an L10 ordered FeCu alloyWe have calculated the electronic structure of the tetragonal L10 ordered FeCu by solving self-consistently a tight-binding Hamiltonian for s, p and d electrons. We have found by total energy…Daniel Errandonea·Jun 7, 1997SaveLearn
Spin-Peierls Dimerization of a s=1/2 Heisenberg Antiferromagnet on Square LatticeDimerization of a spin-half Heisenberg antiferromagnet on a square lattice is investigated by taking unexpanded exchange couplings. Several dimerized configurations are considered some of which are…Aiman Al-Omari, A. H. Nayyar·Jun 6, 1997SaveLearn
Dynamics of viscous amphiphilic films supported by elastic solid substratesThe dynamics of amphiphilic films deposited on a solid surface is analyzed for the case when shear oscillations of the solid surface are excited. The two cases of surface- and bulk shear waves are…M. V. Voinova, M. Jonson, B. Kasemo·Jun 6, 1997SaveLearn
Emergence of quantum chaos in finite interacting Fermi systemsWe study the level spacing statistics P(s) in many-body Fermi systems and determine a critical two-body interaction strength Uc at which a crossover from Poisson to Wigner-Dyson statistics takes…Ph. Jacquod, D. L. Shepelyansky·Jun 5, 1997SaveLearn
Monte Carlo Simulation of Magnetization Reversal in Fe Sesquilayers on W(110)Iron sesquilayers grown at room temperature on W(110) exhibit a pronounced coercivity maximum near a coverage of 1.5 atomic monolayers. On lattices which faithfully reproduce the morphology of the…M. Kolesik, M. A. Novotny, P. A. Rikvold·Jun 4, 1997SaveLearn
Slow modes in passive advectionThe anomalous scaling in the Kraichnan model of advection of the passive scalar by a random velocity field with non-smooth spatial behavior is traced down to the presence of slow resonance-type…Denis Bernard, Krzysztof Gawedzki, Antti Kupiainen·Jun 4, 1997SaveLearn
Functional Integral approach to quasi-particles in Fermi Liquid theoryIn this paper we propose a new way of organizing many-body perturbation theory in the Path-integral formulation where a set of quasi-particle wave-functionals ψ's are introduced and are…Tai-Kai Ng·Jun 4, 1997SaveLearn
Nanoscale Field-Effect Transistors: An Ultimate Size AnalysisWe have used a simple, analytically solvable model to analyze the characteristic s of dual-gate metal-oxide-semiconductor field-effect transistors (MOSFETs) with 10-nm-scale channel length L. The…F. G. Pikus, K. K. Likharev·Jun 3, 1997SaveLearn
Conductance of a Finite Quantum Wire Connected to ReservoirsWe study a finite quantum wire connected to external leads, and show that the conductance of the system significantly depends upon the length of the quantum wire and the position of the impurity in…Yu-Liang Liu·Jun 3, 1997SaveLearn
Low-temperature behavior of a Magnetic Impurity in a Heisenberg ChainUsing the bosonization technique, we have studied a spin-1/2 magnetic impurity in Heisenberg chain, and shown that the impurity specific heat and spin susceptibility have an anomalous temperature…Yu-Liang Liu·Jun 3, 1997SaveLearn