2,060 research outputs found

    Ground-State and Domain-Wall Energies in the Spin-Glass Region of the 2D ±J\pm J Random-Bond Ising Model

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    The statistics of the ground-state and domain-wall energies for the two-dimensional random-bond Ising model on square lattices with independent, identically distributed bonds of probability pp of Jij=−1J_{ij}= -1 and (1−p)(1-p) of Jij=+1J_{ij}= +1 are studied. We are able to consider large samples of up to 3202320^2 spins by using sophisticated matching algorithms. We study L×LL \times L systems, but we also consider L×ML \times M samples, for different aspect ratios R=L/MR = L / M. We find that the scaling behavior of the ground-state energy and its sample-to-sample fluctuations inside the spin-glass region (pc≤p≤1−pcp_c \le p \le 1 - p_c) are characterized by simple scaling functions. In particular, the fluctuations exhibit a cusp-like singularity at pcp_c. Inside the spin-glass region the average domain-wall energy converges to a finite nonzero value as the sample size becomes infinite, holding RR fixed. Here, large finite-size effects are visible, which can be explained for all pp by a single exponent ω≈2/3\omega\approx 2/3, provided higher-order corrections to scaling are included. Finally, we confirm the validity of aspect-ratio scaling for R→0R \to 0: the distribution of the domain-wall energies converges to a Gaussian for R→0R \to 0, although the domain walls of neighboring subsystems of size L×LL \times L are not independent.Comment: 11 pages with 15 figures, extensively revise

    Random Field and Random Anisotropy Effects in Defect-Free Three-Dimensional XY Models

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    Monte Carlo simulations have been used to study a vortex-free XY ferromagnet with a random field or a random anisotropy on simple cubic lattices. In the random field case, which can be related to a charge-density wave pinned by random point defects, it is found that long-range order is destroyed even for weak randomness. In the random anisotropy case, which can be related to a randomly pinned spin-density wave, the long-range order is not destroyed and the correlation length is finite. In both cases there are many local minima of the free energy separated by high entropy barriers. Our results for the random field case are consistent with the existence of a Bragg glass phase of the type discussed by Emig, Bogner and Nattermann.Comment: 10 pages, including 2 figures, extensively revise

    Finite-Size Scaling Critical Behavior of Randomly Pinned Spin-Density Waves

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    We have performed Monte Carlo studies of the 3D XYXY model with random uniaxial anisotropy, which is a model for randomly pinned spin-density waves. We study L×L×LL \times L \times L simple cubic lattices, using LL values in the range 16 to 64, and with random anisotropy strengths of D/2JD / 2 J = 1, 2, 3, 6 and ∞\infty. There is a well-defined finite temperature critical point, TcT_c, for each these values of D/2JD / 2 J. We present results for the angle-averaged magnetic structure factor, S(k)S (k) at TcT_c for L=64L = 64. We also use finite-size scaling analysis to study scaling functions for the critical behavior of the specific heat, the magnetization and the longitudinal magnetic susceptibility. Good data collapse of the scaling functions over a wide range of TT is seen for D/2JD / 2 J = 6 and ∞\infty. For our finite values of D/2JD / 2 J the scaled magnetization function increases with LL below TcT_c, and appears to approach an LL-independent limit for large LL. This suggests that the system is ferromagnetic below TcT_c.Comment: 21 pages in single column format, 20 .eps files, revised and expanded, errors corrected, submitted to PR

    Background gauge invariance in the antifield formalism for theories with open gauge algebras

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    We show that any BRST invariant quantum action with open or closed gauge algebra has a corresponding local background gauge invariance. If the BRST symmetry is anomalous, but the anomaly can be removed in the antifield formalism, then the effective action possesses a local background gauge invariance. The presence of antifields (BRST sources) is necessary. As an example we analyze chiral W3W_3 gravity.Comment: 17pp., Latex, mispelling in my name! corrected, no other change

    Regularisation, the BV method, and the antibracket cohomology

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    We review the Lagrangian Batalin--Vilkovisky method for gauge theories. This includes gauge fixing, quantisation and regularisation. We emphasize the role of cohomology of the antibracket operation. Our main example is d=2d=2 gravity, for which we also discuss the solutions for the cohomology in the space of local integrals. This leads to the most general form for the action, for anomalies and for background charges.Comment: 12 pages, LaTeX, Preprint-KUL-TF-94/2

    Compression of Atomic Phase Space Using an Asymmetric One-Way Barrier

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    We show how to construct asymmetric optical barriers for atoms. These barriers can be used to compress phase space of a sample by creating a confined region in space where atoms can accumulate with heating at the single photon recoil level. We illustrate our method with a simple two-level model and then show how it can be applied to more realistic multi-level atoms

    Domain wall entropy of the bimodal two-dimensional Ising spin glass

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    We report calculations of the domain wall entropy for the bimodal two-dimensional Ising spin glass in the critical ground state. The L * L system sizes are large with L up to 256. We find that it is possible to fit the variance of the domain wall entropy to a power function of L. However, the quality of the data distributions are unsatisfactory with large L > 96. Consequently, it is not possible to reliably determine the fractal dimension of the domain walls.Comment: 4 pages, 2 figures, submitted to PR

    Power-law correlations and orientational glass in random-field Heisenberg models

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    Monte Carlo simulations have been used to study a discretized Heisenberg ferromagnet (FM) in a random field on simple cubic lattices. The spin variable on each site is chosen from the twelve [110] directions. The random field has infinite strength and a random direction on a fraction x of the sites of the lattice, and is zero on the remaining sites. For x = 0 there are two phase transitions. At low temperatures there is a [110] FM phase, and at intermediate temperature there is a [111] FM phase. For x > 0 there is an intermediate phase between the paramagnet and the ferromagnet, which is characterized by a |k|^(-3) decay of two-spin correlations, but no true FM order. The [111] FM phase becomes unstable at a small value of x. At x = 1/8 the [110] FM phase has disappeared, but the power-law correlated phase survives.Comment: 8 pages, 12 Postscript figure

    Effect of Anode Dielectric Coating on Hall Thruster Operation

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    An interesting phenomenon observed in the near-anode region of a Hall thruster is that the anode fall changes from positive to negative upon removal of the dielectric coating, which is produced on the anode surface during the normal course of Hall thruster operation. The anode fall might affect the thruster lifetime and acceleration efficiency. The effect of the anode coating on the anode fall is studied experimentally using both biased and emissive probes. Measurements of discharge current oscillations indicate that thruster operation is more stable with the coated anode
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