The Structure of Barium in the hcp Phase Under High PressureRecent experimental results on two hcp phases of barium under high pressure show interesting variation of the lattice parameters. They are here interpreted in terms of electronic structure…W. -S. Zeng, O. Jepsen, V. Heine·Aug 26, 1996SaveLearn
Spin liquid in 3D Kondo lattice. High temperature regimeThe mechanism explaining the key role of AFM correlations in formation of the heavy fermion state is offered. It is shown that in the case of (T*-TN)/TN << 1 the critical spin fluctuations…K. A. Kikoin, M. N. Kiselev, A. S. Mishchenko·Aug 26, 1996SaveLearn
Screening effects in superconductorsThe partition function of the Hubbard model with local attraction and long range Coulomb repulsion between electrons is written as a functional integral with an action A involving a pairing field…Massimiliano Capezzali, Daniel Ariosa, Hans Beck·Aug 26, 1996SaveLearn
Spin and charge gaps in the one-dimensional Kondo-lattice model with Coulomb interaction between conduction electronsThe density-matrix renormalization-group method is applied to the one-dimensional Kondo-lattice model with the Coulomb interaction between the conduction electrons. The spin and charge gaps are…N. Shibata, T. Nishino, K. Ueda et al.·Aug 26, 1996SaveLearn
Spectral form factor in a random matrix theoryIn the theory of disordered systems the spectral form factor S(τ), the Fourier transform of the two-level correlation function with respect to the difference of energies, is linear for τ<τc and…E. Brézin, S. Hikami·Aug 26, 1996SaveLearn
Form-factors computation of Friedel oscillations in Luttinger liquidsWe show how to analytically determine for g≤ 1/2 the "Friedel oscillations" of charge density by a single impurity in a 1D Luttinger liquid of spinless electrons.F. Lesage, H. Saleur·Aug 25, 1996SaveLearn
New Universality Class at the Superconductor--Insulator TransitionWe study dynamic properties of thin films near the superconductor - insulator transition. We formulate the problem in a phase representation. The key new feature of our model is the assumption of a…Karl-Heinz Wagenblast, Anne van Otterlo, Gerd Schön et al.·Aug 24, 1996SaveLearn
Variational state based on the Bethe ansatz solution and a correlated singlet liquid state in the one-dimensional t-J modelThe one-dimensional t-J model is investigated by the variational Monte Carlo method. A variational wave function based on the Bethe ansatz solution is newly proposed, where the spin-charge separation…Kenji Kobayashi, Chikaomi Ohe, Kaoru Iguchi·Aug 24, 1996SaveLearn
Fragmentation phase transition in atomic clusters I --- Microcanonical thermodynamicsHere we first develop the thermodynamics of microcanonical phase transitions of first and second order in systems which are thermodynamically stable in the sense of van Hove. We show how both kinds…D. H. E. Gross, M. E. Madjet, O. Schapiro·Aug 23, 1996SaveLearn
Bulk Versus Edge in the Quantum Hall EffectThe manifestation of the bulk quantum Hall effect on edge is the chiral anomaly. The chiral anomaly is the underlying principle of the ``edge approach'' of quantum Hall effect. In that…Y. -C. Kao, D. -H. Lee·Aug 23, 1996SaveLearn
Spin Splitting and Weak Localization in (110) GaAs/AlGaAs Quantum WellsWe investigate experimentally and theoretically the spin-orbit effects on the weak localization in a (110) GaAs 2-dimensional electron gas (2DEG). We analyze the role of two different terms in the…T. Hassenkam, S. Pedersen, K. Baklanov et al.·Aug 23, 1996SaveLearn
NMR in copper-Oxide MetalsThe anomalous part of the NMR relaxation rate of coppernuclei in the normal state of copper-oxide metals is calculated using the orbital magnetic parts of the fluctuations derived in a recent theory…C. M. Varma·Aug 23, 1996SaveLearn
Cooperative Chiral Order in Copolymers of Chiral and Achiral UnitsPolyisocyanates can be synthesized with chiral and achiral pendant groups distributed randomly along the chains. The overall chiral order, measured by optical activity, is strongly cooperative and…J. V. Selinger, R. L. B. Selinger·Aug 23, 1996SaveLearn
Mott Transition in Degenerate Hubbard Models: Application to Doped FullerenesThe Mott-Hubbard transition is studied for a Hubbard model with orbital degeneracy N, using a diffusion Monte-Carlo method. Based on general arguments, we conjecture that the Mott-Hubbard transition…Olle Gunnarsson, Erik Koch, Richard M. Martin·Aug 23, 1996SaveLearn
Frustration induced Raman scattering in CuGeO3We present experimental data for the Raman intensity in the spin-Peierls compound CuGeO3 and theoretical calculations from a one-dimensional frustrated spin model. The theory is based on (a) exact…V. N. Muthukumar, Claudius Gros, Wolfgang Wenzel et al.·Aug 23, 1996SaveLearn
Is there a Phase Transition to the Flux Lattice State?The sharp drops in the resistance and magnetization which are usually attributed to a phase transition from the vortex liquid state to a crystal state are explained instead as a crossover between…M. A. Moore·Aug 23, 1996SaveLearn
RKKY interaction and Kondo screening cloud for correlated electronsThe RKKY law and the Kondo screening cloud around a magnetic impurity are investigated for correlated electrons in 1D (Luttinger liquid). We find slow algebraic distance dependences, with a crossover…Reinhold Egger, Herbert Schoeller·Aug 23, 1996SaveLearn
Phase transition in a spring-block model of surface fractureA simple and robust spring-block model obeying threshold dynamics is introduced to study surface fracture of an overlayer subject to stress induced by adhesion to a substrate. We find a novel phase…Kwan-tai Leung, Joergen Vitting Andersen·Aug 23, 1996SaveLearn
Electric field scaling at a B=0 metal-insulator transition in two dimensionsThe non-linear (electric field-dependent) resistivity of the 2D electron system in silicon exhibits scaling as a function of electric field and electron density in both the metallic and insulating…S. V. Kravchenko, D. Simonian, M. P. Sarachik et al.·Aug 22, 1996SaveLearn
Spin ladders with nonmagnetic impuritiesWe investigate antiferromagnetic spin ladders with nonmagnetic impurities by variational and numerical (Lanczos and DMRG) methods. The interaction between the two unpaired spins opposite to the…H. -J. Mikeska, U. Neugebauer, U. Schollwoeck·Aug 22, 1996SaveLearn
The Upper Critical Dimension of the KPZ EquationThe strong-coupling regime of Kardar-Parisi-Zhang surface growth driven by short-ranged noise has an upper critical dimension d> less or equal to four (where the dynamic exponent z takes the value z…Michael Lassig, Harald Kinzelbach·Aug 22, 1996SaveLearn
Supercurrent in a mesoscopic proximity wireRecent experiments on the proximity induced supercurrent in mesoscopic normal wires revealed a surprising temperature dependence. They suggest clean-limit behavior although the wires are strongly…Frank K. Wilhelm, Andrei D. Zaikin, Gerd Schoen·Aug 22, 1996SaveLearn
Chaotic Scattering with Resonance EnhancementThe passage of light or of electrons through a disordered medium is modified in the presence of resonances. We describe a simple model for this problem, and present first results.B. Elattari, V. Kagalovsky, H. A. Weidenmueller·Aug 22, 1996SaveLearn
Continuum Monte Carlo Simulation at Constant Pressure of Stiff Chain Molecules at SurfacesContinuum Monte-Carlo simulations at constant pressure are performed on short chain molecules at surfaces. The rodlike chains, consisting of seven effective monomers, are attached at one end to a…R. Hilfer, F. M. Haas·Aug 22, 1996SaveLearn
Ground State Entropy and the q=3 Potts Antiferromagnet on the Honeycomb LatticeWe study the q-state Potts antiferromagnet with q=3 on the honeycomb lattice. Using an analytic argument together with a Monte Carlo simulation, we conclude that this model is disordered for all…Robert Shrock, Shan-Ho Tsai·Aug 21, 1996SaveLearn