51,030 research outputs found

    Screening in Ionic Systems: Simulations for the Lebowitz Length

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    Simulations of the Lebowitz length, ξL(T,ρ)\xi_{\text{L}}(T,\rho), are reported for t he restricted primitive model hard-core (diameter aa) 1:1 electrolyte for densi ties ρ4ρc\rho\lesssim 4\rho_c and TcT40TcT_c \lesssim T \lesssim 40T_c. Finite-size eff ects are elucidated for the charge fluctuations in various subdomains that serve to evaluate ξL\xi_{\text{L}}. On extrapolation to the bulk limit for T10TcT\gtrsim 10T_c the low-density expansions (Bekiranov and Fisher, 1998) are seen to fail badly when ρ>1/10ρc\rho > {1/10}\rho_c (with ρca30.08\rho_c a^3 \simeq 0.08). At highe r densities ξL\xi_{\text{L}} rises above the Debye length, \xi_{\text{D}} \prop to \sqrt{T/\rho}, by 10-30% (upto ρ1.3ρc\rho\simeq 1.3\rho_c); the variation is portrayed fairly well by generalized Debye-H\"{u}ckel theory (Lee and Fisher, 19 96). On approaching criticality at fixed ρ\rho or fixed TT, ξL(T,ρ)\xi_{\text{L}}(T, \rho) remains finite with ξLc0.30a1.3ξDc\xi_{\text{L}}^c \simeq 0.30 a \simeq 1.3 \xi_{\text {D}}^c but displays a weak entropy-like singularity.Comment: 4 pages 5 figure

    Fractal Droplets in Two Dimensional Spin Glasses

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    The two-dimensional Edwards-Anderson model with Gaussian bond distribution is investigated at T=0 with a numerical method. Droplet excitations are directly observed. It turns out that the averaged volume of droplets is proportional to l^D with D = 1.80(2) where l is the spanning length of droplets, revealing their fractal nature. The exponent characterizing the l dependence of the droplet excitation energy is estimated to be -0.42(4), clearly different from the stiffness exponent for domain wall excitations.Comment: 4 pages 4 figure

    Current-voltage scaling of chiral and gauge-glass models of two-dimensional superconductors

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    The scaling behavior of the current-voltage characteristics of chiral and gauge glass models of disordered superconductors, are studied numerically, in two dimensions. For both models, the linear resistance is nonzero at finite temperatures and the scaling analysis of the nonlinear resistivity is consistent with a phase transition at T=0 temperature characterized by a diverging correlation length ξTνT\xi \propto T^{-\nu_{T}} and thermal critical exponent νT\nu_{T}. The values of νT\nu_{T}, however, are found to be different for the chiral and gauge glass models, suggesting different universality classes, in contrast to the result obtained recently in three dimensions.Comment: 4 pages, 4 figures (included), to appear in Phys. Rev.

    When is diabetes distress clinically meaningful?: establishing cut points for the Diabetes Distress Scale.

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    ObjectiveTo identify the pattern of relationships between the 17-item Diabetes Distress Scale (DDS17) and diabetes variables to establish scale cut points for high distress among patients with type 2 diabetes.Research design and methodsRecruited were 506 study 1 and 392 study 2 adults with type 2 diabetes from community medical groups. Multiple regression equations associated the DDS17, a 17-item scale that yields a mean-item score, with HbA(1c), diabetes self-efficacy, diet, and physical activity. Associations also were undertaken for the two-item DDS (DDS2) screener. Analyses included control variables, linear, and quadratic (curvilinear) DDS terms.ResultsSignificant quadratic effects occurred between the DDS17 and each diabetes variable, with increases in distress associated with poorer outcomes: study 1 HbA(1c) (P < 0.02), self-efficacy (P < 0.001), diet (P < 0.001), physical activity (P < 0.04); study 2 HbA(1c) (P < 0.03), self-efficacy (P < 0.004), diet (P < 0.04), physical activity (P = NS). Substantive curvilinear associations with all four variables in both studies began at unexpectedly low levels of DDS17: the slope increased linearly between scores 1 and 2, was more muted between 2 and 3, and reached a maximum between 3 and 4. This suggested three patient subgroups: little or no distress, <2.0; moderate distress, 2.0-2.9; high distress, ≥3.0. Parallel findings occurred for the DDS2.ConclusionsIn two samples of type 2 diabetic patients we found a consistent pattern of curvilinear relationships between the DDS and HbA(1c), diabetes self-efficacy, diet, and physical activity. The shape of these relationships suggests cut points for three patient groups: little or no, moderate, and high distress

    Thermodynamic Casimir effects involving interacting field theories with zero modes

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    Systems with an O(n) symmetrical Hamiltonian are considered in a dd-dimensional slab geometry of macroscopic lateral extension and finite thickness LL that undergo a continuous bulk phase transition in the limit LL\to\infty. The effective forces induced by thermal fluctuations at and above the bulk critical temperature Tc,T_{c,\infty} (thermodynamic Casimir effect) are investigated below the upper critical dimension d=4d^*=4 by means of field-theoretic renormalization group methods for the case of periodic and special-special boundary conditions, where the latter correspond to the critical enhancement of the surface interactions on both boundary planes. As shown previously [\textit{Europhys. Lett.} \textbf{75}, 241 (2006)], the zero modes that are present in Landau theory at Tc,T_{c,\infty} make conventional RG-improved perturbation theory in 4ϵ4-\epsilon dimensions ill-defined. The revised expansion introduced there is utilized to compute the scaling functions of the excess free energy and the Casimir force for temperatures T\geqT_{c,\infty} as functions of LL/ξ\mathsf{L}\equiv L/\xi_\infty, where ξ\xi_\infty is the bulk correlation length. Scaling functions of the LL-dependent residual free energy per area are obtained whose L0\mathsf{L}\to0 limits are in conformity with previous results for the Casimir amplitudes ΔC\Delta_C to O(ϵ3/2)O(\epsilon^{3/2}) and display a more reasonable small-L\mathsf{L} behavior inasmuch as they approach the critical value ΔC\Delta_C monotonically as L0\mathsf{L}\to 0.Comment: 23 pages, 10 figure

    Fluctuating loops and glassy dynamics of a pinned line in two dimensions

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    We represent the slow, glassy equilibrium dynamics of a line in a two-dimensional random potential landscape as driven by an array of asymptotically independent two-state systems, or loops, fluctuating on all length scales. The assumption of independence enables a fairly complete analytic description. We obtain good agreement with Monte Carlo simulations when the free energy barriers separating the two sides of a loop of size L are drawn from a distribution whose width and mean scale as L^(1/3), in agreement with recent results for scaling of such barriers.Comment: 11 pages, 4 Postscript figure

    New varieties top 1967 yield tests

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    LARGE gains can result from using improved cereal varieties and in recent years activity in breeding varieties adapted to local conditions has increased. The varieties available and their suitability for different areas and conditions need constant review

    Varieties and time of sowing

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    THE extent to which seasonal conditions favour the various stages of plant development has a marked effect on cereal yields. Because varieties differ in their development they react in different ways to a particular seasonal pattern

    Probability distribution of the order parameter in the directed percolation universality class

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    The probability distributions of the order parameter for two models in the directed percolation universality class were evaluated. Monte Carlo simulations have been performed for the one-dimensional generalized contact process and the Domany-Kinzel cellular automaton. In both cases, the density of active sites was chosen as the order parameter. The criticality of those models was obtained by solely using the corresponding probability distribution function. It has been shown that the present method, which has been successfully employed in treating equilibrium systems, is indeed also useful in the study of nonequilibrium phase transitions.Comment: 6 pages, 4 figure

    Cereal yield tests in 1966

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    FARMER\u27S main guide in his choice of a cereal variety is its capacity to produce high overall yields of saleable grain over many years in a particular district
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