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. 2014 Apr 4;4:4440. doi: 10.1038/srep04440

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(a) The size-dependent probability distribution Q_N for the rescaled o.p. x, calculated for T_c(N), P_c(N) and B(N), has a symmetric shape that approaches continuously (from N = 2500, symbols at the top at x = 0, to N = 40000, symbols at the bottom) the limiting form for the 2D Ising universality class (full blue line) and differs from the 3D Ising universality class case (full black line). Error bars are smaller than the symbols size. (b) The size-dependent LLCP temperature T_c(N) and (c) pressure P_c(N) (symbols), resulting from our best-fit of Q_N, extrapolate to and , respectively, following the expected linear behaviors (lines). (d) The normalization factor B(N) (symbols) follows the power law function (dashed line) ∝ N^β/dν. We use the d = 2 Ising critical exponents: θ = 2 (correction to scaling), ν = 1 and β = 1/8 (both defined in the text).

Inline graphic — (a) The size-dependent probability distribution Q_N for the rescaled o.p. x, calculated for T_c(N), P_c(N) and B(N), has a symmetric shape that approaches continuously (from N = 2500, symbols at the top at x = 0, to N = 40000, symbols at the bottom) the limiting form for the 2D Ising universality class (full blue line) and differs from the 3D Ising universality class case (full black line). Error bars are smaller than the symbols size. (b) The size-dependent LLCP temperature T_c(N) and (c) pressure P_c(N) (symbols), resulting from our best-fit of Q_N, extrapolate to and , respectively, following the expected linear behaviors (lines). (d) The normalization factor B(N) (symbols) follows the power law function (dashed line) ∝ N^β/dν. We use the d = 2 Ising critical exponents: θ = 2 (correction to scaling), ν = 1 and β = 1/8 (both defined in the text).