The Fermion Chern-Simons Gauge Theory of Fractional Quantum Hall Effect for Electromagnetic Polarization TensorUnlike an earlier theory, by avoiding both the electromagnetic gauge field shift and the assumption of the zero average of electromagnetic field fluctuation the fermion Chern-Simons gauge theory is…Tae-Hyoung Gimm, Sung-Ho Suck Salk·Jun 11, 1996SaveLearn
Complete Wiener-Hopf Solution of the X-Ray Edge ProblemWe present a complete solution of the soft x-ray edge problem within a field-theoretic approach based on the Wiener-Hopf infinite-time technique. We derive for the first time within this approach…V. Janis·Jun 11, 1996SaveLearn
Mesoscopic Effects in the Fractional Quantum Hall Regime: Chiral Luttinger versus Fermi LiquidWe study tunneling through an edge state formed around an antidot in the fractional quantum Hall regime using Wen's chiral Luttinger liquid theory extended to include mesoscopic effects. We…Michael R. Geller, Daniel Loss, George Kirczenow·Jun 11, 1996SaveLearn
Spatial organization in cyclic Lotka-Volterra systemsWe study the evolution of a system of N interacting species which mimics the dynamics of a cyclic food chain. On a one-dimensional lattice with N<5 species, spatial inhomogeneities develop…L. Frachebourg, P. L. Krapivsky, E. Ben-Naim·Jun 11, 1996SaveLearn
Josephson Effect in Unconventional SuperconductorsIn this letter we present a simple relation, that allows one to predict the Josephson current between two unconventional superconductors with arbitrary band-structure and pairing symmetry. We…Supriyo Datta, Manoj P. Samanta·Jun 10, 1996SaveLearn
Two-spinon dynamic structure factor of the one-dimensional S=1/2 Heisenberg antiferromagnetThe exact expression derived by Bougourzi, Couture, and Kacir for the 2-spinon contribution to the dynamic spin structure factor Szz(q,ω) of he one-dimensional S=1/2 Heisenberg antiferromagnet…Michael Karbach, Gerhard Müller, A. Hamid Bougourzi·Jun 10, 1996SaveLearn
Shape Phase Transition of Polyampholytes in Two DimensionsWe have studied the transition in shape of two dimensional polyampholytes using Monte Carlo simulation. We observe that polymers with randomly charged monomers get into a globular shape at lower…M. R. Ejtehadi, S. Rouhani·Jun 10, 1996SaveLearn
The Surface Region of Superfluid 4He as a Dilute Bose-Condensed GasIn the low-density surface region of superfluid 4He, the atoms are far apart and collisions can be ignored. The only effect of the interactions is from the long-range attractive Hartree potential…A. Griffin, S. Stringari·Jun 10, 1996SaveLearn
Avalanches, Scaling and Coherent NoiseWe present a simple model of a dynamical system driven by externally-imposed coherent noise. Although the system never becomes critical in the sense of possessing spatial correlations of arbitrarily…M. E. J. Newman, Kim Sneppen·Jun 10, 1996SaveLearn
Momentum-Dependent Charge Transfer Excitations in Sr2CuO2Cl2 - Angle Resolved Electron Energy Loss SpectroscopyElectron-hole pair excitations in the insulating cuprates Sr2CuO2Cl2 were investigated by angle-resolved electron energy loss spectroscopy. The optically allowed and optically forbidden…Y. Y. Wang, F. C. Zhang, V. P. Dravid et al.·Jun 10, 1996SaveLearn
Bosonization in the two-channel Kondo modelThe bosonization of the S=1/2 anisotropic two-channel Kondo model is shown to yield two equivalent representations of the original problem. In a straight forward extension of the Emery-Kivelson…A. J. Schofield·Jun 10, 1996SaveLearn
Phase of Aharonov-Bohm oscillations in conductance of mesoscopic systemsMotivated by a recent experiment we analyze in detail the phase of Aharonov-Bohm oscillations across a 1D ring with a stub coupled to one of its arms, in the presence of a magnetic flux. We…P. Singha Deo, A. M. Jayannavar·Jun 10, 1996SaveLearn
Neutron Compton ScatteringNeutron Compton scattering measurements have the potential to provide direct information about atomic momentum distributions and adiabatic energy surfaces in condensed matter. First applied to…Greg Watson·Jun 10, 1996SaveLearn
Glassy behaviour in disordered systems with non-relaxational dynamicsWe show that a family of disordered systems with non-relaxational dynamics may exhibit ``glassy'' behavior at nonzero temperature, although such a behavior appears to be ruled out by a…Leticia F. Cugliandolo, Jorge Kurchan, Pierre Le Doussal et al.·Jun 10, 1996SaveLearn
Surprises in the Orbital Magnetic Moment and g-Factor of the Dynamic Jahn-Teller Ion C60-We calculate the magnetic susceptibility and g-factor of the isolated C60- ion at zero temperature, with a proper treatment of the dynamical Jahn-Teller effect, and of the associated orbital…Erio Tosatti, Nicola Manini, Olle Gunnarsson·Jun 10, 1996SaveLearn
Surface Magnetisation and Surface Correlations in Aperiodic Ising ModelsWe consider the surface critical behaviour of diagonally layered Ising models on the square lattice where the inter-layer couplings follow some aperiodic sequence. The surface magnetisation is…Ferenc Igloi, Peter Lajko·Jun 10, 1996SaveLearn
Interface Fluctuations on a Hierarchical LatticeWe consider interface fluctuations on a two-dimensional layered lattice where the couplings follow a hierarchical sequence. This problem is equivalent to the diffusion process of a quantum particle…Ferenc Igloi, Ferenc Szalma·Jun 10, 1996SaveLearn
Dynamics in the dimerised and high field incommensurate phase of CuGeO3Temperature (2.3<T<40\ K) and magnetic field (0<B<17\ T) dependent far infrared absorption spectroscopy on the spin-Peierls coumpound CuGeO3\ has revealed several new absorption processes in…P. H. M. van Loosdrecht, S. Huant, G. Martinez et al.·Jun 10, 1996SaveLearn
The Ngai model of relaxation: An alternative for the study of an interacting system of small particlesIt is shown that the Ngai model of relaxation accounts for the main experimental results of the magnetic relaxation in an assembly of interacting fine particles.J. Castro·Jun 10, 1996SaveLearn
Random Walks through the Ensemble: Linking Spectral Statistics with Wavefunction Correlations in Disordered MetalsWe use a random walk in the ensemble of impurity configurations to generate a Brownian motion model for energy levels in disordered conductors. Treating arc-length along the random walk as fictitous…J. T. Chalker, Igor V. Lerner, Robert A. Smith·Jun 10, 1996SaveLearn
Matrix-Product States for a One-Dimensional Lattice Gas with Parallel DynamicsThe hopping motion of classical particles on a chain coupled to reservoirs at both ends is studied for parallel dynamics with arbitrary probabilities. The stationary state is obtained in the form of…A. Honecker, I. Peschel·Jun 10, 1996SaveLearn
Equilibrium and off-equilibrium simulations of the 4d Gaussian spin glassIn this paper we study the on and off-equilibrium properties of the four dimensional Gaussian spin glass. In the static case we determine with more precision that in previous simulations both the…Giorgio Parisi, Federico Ricci-Tersenghi, Juan J. Ruiz-Lorenzo·Jun 9, 1996SaveLearn
NiO Exchange Bias Layers Grown by Direct Ion Beam Sputtering of a Nickel Oxide TargetA new process for fabricating NiO exchange bias layers has been developed. The process involves the direct ion beam sputtering (IBS) of a NiO target. The process is simpler than other deposition…Richard P. Michel, A. Chaiken, Young K. Kim et al.·Jun 9, 1996SaveLearn
On the 3n+l Quantum Number in the Cluster ProblemIt has recently been suggested that an exactly solvable problem characterized by a new quantum number may underlie the electronic shell structure observed in the mass spectra of medium-sized sodium…Erik Koch·Jun 8, 1996SaveLearn
Interacting Arrays of Steps and Lines in Random MediaThe phase diagram of two interacting planar arrays of directed lines in random media is obtained by a renormalization group analysis. The results are discussed in the contexts of the roughening of…J. Kierfeld, T. Hwa·Jun 8, 1996SaveLearn