1,721,030 research outputs found

    The critical behavior of 3D Ising glass models: universality and scaling corrections

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    We perform high-statistics Monte Carlo simulations of three three-dimensional Ising spin-glass models: the +-J Ising model for two values of the disorder parameter p, p=1/2 and p=0.7, and the bond-diluted +-J model for bond-occupation probability p_b = 0.45. A finite-size scaling analysis of the quartic cumulants at the critical point shows conclusively that these models belong to the same universality class and allows us to estimate the scaling-correction exponent omega related to the leading irrelevant operator, omega=1.0(1). We also determine the critical exponents nu and eta. Taking into account the scaling corrections, we obtain nu=2.53(8) and eta=-0.384(9)

    Anisotropic perturbations in three-dimensional O(N)-symmetric vector models

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    We investigate the effects of anisotropic perturbations in three-dimensional O(N)-symmetric vector models. In order to assess their relevance for the critical behavior, we determine the renormalization-group dimensions of the anisotropic perturbations associated with the first few spin values of the representations of the O(N) group, because the lowest spin values give rise to the most important effects. In particular, we determine them up to spin 4 for N = 2, 3, 4, by finite-size analyses of Monte Carlo simulations of lattice O(N) models, achieving a significant improvement of their accuracy. These results are relevant for several physical systems, such as density-wave systems, magnets with cubic symmetry, and multicritical phenomena arising from the competition of different order parameters

    Critical behavior of two-dimensional fully frustrated XY systems

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    We study the phase diagram of the two-dimensional fully frustrated XY model (FFXY) and of two related models, a lattice discretization of the Landau-Ginzburg-Wilson Hamiltonian for the critical modes of the FFXY model, and a coupled Ising-XY model. We present Monte Carlo simulations on square lattices L×LL\times L, L103L\lesssim 10^3. We show that the low-temperature phase of these models is controlled by the same line of Gaussian fixed points as in the standard XY model. We find that, if a model undergoes a unique transition by varying temperature, then the transition is of first order. In the opposite case we observe two very close transitions: a transition associated with the spin degrees of freedom and, as temperature increases, a transition where chiral modes become critical. If they are continuous, they belong to the Kosterlitz-Thouless and to the Ising universality class, respectively. Ising and Kosterlitz-Thouless behavior is observed only after a preasymptotic regime, which is universal to some extent. In the chiral case, the approach is nonmonotonic for most observables, and there is a wide region in which finite-size scaling is controlled by an effective exponent νeff0.8\nu_{\rm eff} \approx 0.8. This explains the result ν0.8\nu\approx 0.8 of many previous studies using smaller lattices

    Magnetic-glassy multicritical behavior of the three-dimensional +- J Ising model

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    We consider the three-dimensional ±J\pm J model defined on a simple cubic lattice and study its behavior close to the multicritical Nishimori point where the paramagnetic-ferromagnetic, the paramagnetic-glassy, and the ferromagnetic-glassy transition lines meet in the T-p phase diagram (p characterizes the disorder distribution and gives the fraction of ferromagnetic bonds). For this purpose we perform Monte Carlo simulations on cubic lattices of size L32L\le 32 and a finite-size scaling analysis of the numerical results. The magnetic-glassy multicritical point is found at p=0.76820(4)p^*=0.76820(4), along the Nishimori line given by 2p1=Tanh(J/T)2p-1={\rm Tanh}(J/T). We determine the renormalization-group dimensions of the operators that control the renormalization-group flow close to the multicritical point, y1=1.02(5)y_1 = 1.02(5), y2=0.61(2)y_2 = 0.61(2), and the susceptibility exponent η=0.114(3)\eta = -0.114(3). The temperature and crossover exponents are ν=1/y2=1.64(5)\nu=1/y_2=1.64(5) and ϕ=y1/y2=1.67(10)\phi=y_1/y_2 = 1.67(10), respectively. We also investigate the model-A dynamics, obtaining the dynamic critical exponent z=5.0(5)z = 5.0(5)

    Critical exponents and equation of state of three-dimensional spin models

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    Three-dimensional spin models of the Ising and XY universality classes are studied by a combination of high-temperature expansions and Monte Carlo simulations. Critical exponents are determined to very high precision. Scaling amplitude ratios are computed via the critical equation of state. Our results are compared with other theoretical computations and with experiments, with special emphasis on the lambda transition of 4He
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