Level spectroscopy II - application to the Gaussian model -It was a difficult problem to determine the Gaussian fixed line from the numerical data, because close to the Berezinskii-Kosterlitz-Thouless multicritical point the divergence of the correlation…Kiyohide Nomura, Atsuhiro Kitazawa·Jun 18, 1996SaveLearn
Dynamical Phase Transition in a Driven Disordered Vortex LatticeUsing Langevin dynamics, we have investigated the dynamics of vortices in a disordered two dimensional superconductor subjected to a uniform driving current. The results provide direct numerical…Seungoh Ryu, M. Hellerqvist, S. Doniach et al.·Jun 18, 1996SaveLearn
Exact Friedel oscillations in the g=1/2 Luttinger liquidA single impurity in the 1D Luttinger model creates a local modification of the charge density analogous to the Friedel oscillations. In this paper, we present an exact solution of the case…A. Leclair, F. Lesage, H. Saleur·Jun 17, 1996SaveLearn
A Study of The Formation of Stationary Localized States Due to Nonlinear Impurities Using The Discrete Nonlinear Schrödinger EquationThe Discrete Nonlinear Schrodinger Equation is used to study the formation of stationary localized states due to a single nonlinear impurity in a Caley tree and a dimeric nonlinear impurity…B. C. Gupta, K. Kundu·Jun 17, 1996SaveLearn
Global Persistence Exponent for Critical DynamicsA `persistence exponent' θ is defined for nonequilibrium critical phenomena. It describes the probability, p(t) t-θ, that the global order parameter has not changed sign in the time…S. N. Majumdar, A. J. Bray, S. J. Cornell et al.·Jun 17, 1996SaveLearn
Fractional Quantum Hall Effect in Bilayer Two Dimensional Hole Gas SystemsWe have studied the fractional and integer quantum Hall effect in high mobility double layer 2D hole gas systems. The large hole effective mass inhibits tunneling, allowing us to investigate the…A. R. Hamilton, M. Y. Simmons, F. M. Bolton et al.·Jun 17, 1996SaveLearn
Continuous Versus First Order Transitions in Compressible Diluted MagnetsThe interplay between disorder and compressibility in Ising magnets is studied. Contrary to pure systems in which a weak compressibility drives the transition first order, we find from a…Yonathan Shapir, Serge Galam·Jun 17, 1996SaveLearn
On the presence of mid-gap states in CaV4O9Using exact diagonalizations of finite clusters with up to 32 sites, we study the J1-J2 model on the 1/5 depleted square lattice. Spin-spin correlation functions are consistent with plaquette…Marc Albrecht, Frederic Mila, Didier Poilblanc·Jun 17, 1996SaveLearn
Exact results concerning multifield moduli of two-phase compositesChen has recently shown how the response matrix of a two-phase composite can be written as linear combinations of products of the component matrices. We elaborate on Chen's expansions by deriving…Mordehai Milgrom·Jun 17, 1996SaveLearn
Common trends in the critical behavior of the Ising and directed walk modelsWe consider layered two-dimensional Ising and directed walk models and show that the two problems are inherently related. The information about the zero-field thermodynamical properties of the Ising…F. Igloi, L. Turban·Jun 17, 1996SaveLearn
Diffusion in disordered media as a process with memoryThe problem of a random walk in a disordered media is mapped into a model of a random walk with memory. The latter model, as opposed to the former one, does not make reference to a particular…Michele Vendruscolo, Matteo Marsili·Jun 17, 1996SaveLearn
A Non-linear Sigma-model for Partially Polarized QH-statesWe consider a two-component quantum Hall system within a Landau-Ginzburg theory with two Chern-Simons gauge fields. From this theory we derive a sigma model covariantly coupled to one Chern-Simons…T. H. Hansson, A. Karlhede, J. M. Leinaas·Jun 17, 1996SaveLearn
A note on ferromagnetism in the Hubbard model on the complete graphRecently there have appeared some papers which discuss the existence of ferromagnetism in the Hubbard model defined on the complete graph. At least for the special electron number Ne=N-1, where N…Andreas Mielke, Hal Tasaki·Jun 17, 1996SaveLearn
Randomly inhomogeneous Luttinger liquid: Fluctuations of the tunnel conductanceThe Luttinger liquid in which the concentration of electrons varies randomly with coordinate is considered. We study the fluctuations of the tunnel conductance, caused by the randomness in the…A. Gramada, M. E. Raikh·Jun 16, 1996SaveLearn
Conduction band spin splitting and negative magnetoresistance in A3 B5 heterostructuresThe quantum interference corrections to the conductivity are calculated for an electron gas in asymmetric quantum wells in a magnetic field. The theory takes into account two different types of the…F. G. Pikus, G. E. Pikus·Jun 16, 1996SaveLearn
Weak Localization and Negative Magnetoresistance in Wurtzite-type CrystalsWe have developed a theory of the negative magnetoresistance due to the weak localization in uniaxial wurtzite-type crystals, in which the spin splitting of the conduction band is linear in the wave…F. G. Pikus, G. E. Pikus·Jun 15, 1996SaveLearn
The Kosterlitz-Thouless Transitions on Fluctuating Surface of Genus ZeroWe investigate the Kosterlitz-Thouless transition for hexatic order on a fluctuating spherical surface of genus zero and derive a Coulomb gas Hamiltonian to describe it. In the Coulomb gas…Jeong-Man Park·Jun 14, 1996SaveLearn
Finite temperature correlations in the one-dimensional quantum Ising modelWe extend the form-factors approach to the quantum Ising model at finite temperature. The two point function of the energy is obtained in closed form, while the two point function of the spin is…A. Leclair, F. Lesage, S. Sachdev et al.·Jun 14, 1996SaveLearn
A new non-Fermi liquid fixed pointWe study a new exchange interaction in which the conduction electrons with pseudo spin Sc=3/2 interact with the impurity spin SI=1/2. Due to the overscreening of the impurity spin by higher…Tae-Suk Kim, L. N. Oliveira, D. L. Cox·Jun 14, 1996SaveLearn
Vortex excitation in superfluid 4He: A Diffusion Monte Carlo studyWe present a diffusion Monte Carlo study of a single vortex in two-dimensional superfluid liquid 4He within the fixed node approximation. We use both the Feynman phase and an improved phase which…S. Giorgini, J. Boronat, J. Casulleras·Jun 14, 1996SaveLearn
Properties of Paired Quantum Hall States at ν=2The energetic properties of a paired quantum Hall state at Landau level filling ν=2 are investigated using variational Monte Carlo techniques. Pairing is found to be energetically favorable in…F. G. Pikus, A. M. Tikofsky·Jun 14, 1996SaveLearn
n-atic Order and Continuous Shape Changes of Deformable Surfaces of Genus ZeroWe consider in mean-field theory the continuous development below a second-order phase transition of n-atic tangent plane order on a deformable surface of genus zero with order parameter $ψ=…Jeong-Man Park, T. C. Lubensky, F. C. MacKintosh·Jun 14, 1996SaveLearn
Transfer and Decay of an Exciton Coupled to Vibrations in a DimerTransfer and decay dynamics of an exciton coupled to a polarization vibration in a dimer is investigated in a mixed quantum-classical picture with the exciton decay incorporated by a sink site. Using…Holger Schanz, Ivan Barvik, Bernd Esser·Jun 14, 1996SaveLearn
Nonlinear transverse magnetic moment in anisotropic superconductorsWe consider the nonlinear transverse magnetic moment that arises in the Meissner state of superconductors with strongly anisotropic order parameter. We compute this magnetic moment as a function of…Igor Zutic, Oriol T. Valls·Jun 14, 1996SaveLearn
Relationship Between Structural Fractal and Possible Dynamic Scaling Properties in Protein FoldingIn this letter, the possible dynamic scaling properties of protein molecules in folding are investigated theoretically by assuming that the protein molecules are percolated networks. It is shown that…Liang-Jian Zou, X. G. Gong, Zheng-Gang Zhu·Jun 14, 1996SaveLearn