• Chinese Physics B
  • Vol. 29, Issue 8, (2020)
Guifeng Su1, Xiaowen Li1, Xiaobing Zhang2, and Yi Zhang1、†
Author Affiliations
  • 1Department of Physics, Shanghai Normal University, Shanghai 200234, China
  • 2School of Physics, Nankai University, Tianjin 300071, China
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    DOI: 10.1088/1674-1056/ab8a41 Cite this Article
    Guifeng Su, Xiaowen Li, Xiaobing Zhang, Yi Zhang. Finite density scaling laws of condensation phase transition in zero-range processes on scale-free networks[J]. Chinese Physics B, 2020, 29(8): Copy Citation Text show less
    The scaling relations of the average occupation number mk versus kρδ at δ = 0.2 for different SF network sizes: (a) L = 1000, (b) L = 2000, (c) L = 4000, (d) L = 8000, at various densities ρ = 0.5 (purple open diamonds), ρ = 2 (blue open triangles), ρ = 10 (red open squares), ρ = 50 (green open circles), respectively.
    Fig. 1. The scaling relations of the average occupation number mk versus δ at δ = 0.2 for different SF network sizes: (a) L = 1000, (b) L = 2000, (c) L = 4000, (d) L = 8000, at various densities ρ = 0.5 (purple open diamonds), ρ = 2 (blue open triangles), ρ = 10 (red open squares), ρ = 50 (green open circles), respectively.
    The presence of the finite density effect in the crossover degree ratios kc(ρ)/kc(ρ = 2) versus the parameter δ with an SF network size L = 4000, for various densities ρ = 1 (black open diamonds and solid line), 5 (blue open triangles and solid line), and 10 (red open squares and solid line), respectively. The solid lines correspond to the theoretical calculation and the symbols to the MC simulation data. Note that kc’s do not exist in regime δ > δc (δc = 0.5 is the vertical red dotted dash line) for ρ = 5 and ρ = 10 due to the lower bound of degree kmin, two theoretical dashed lines are only formally drawn in that region.
    Fig. 2. The presence of the finite density effect in the crossover degree ratios kc(ρ)/kc(ρ = 2) versus the parameter δ with an SF network size L = 4000, for various densities ρ = 1 (black open diamonds and solid line), 5 (blue open triangles and solid line), and 10 (red open squares and solid line), respectively. The solid lines correspond to the theoretical calculation and the symbols to the MC simulation data. Note that kc’s do not exist in regime δ > δc (δc = 0.5 is the vertical red dotted dash line) for ρ = 5 and ρ = 10 due to the lower bound of degree kmin, two theoretical dashed lines are only formally drawn in that region.
    Data collapse plot of (a) the average occupation number mk versus kρδc at the transient time t = 210, (b) the evolution of ratio of IPR to its steady state limit, It/I∞, versus t/ρν, with ν = 1 – δ being the dynamic exponent in the relaxation dynamics, at δ = 0.2 for network size L = 4000, and various densities ρ = 0.5 (purple open diamonds), ρ = 2 (blue open triangles), ρ = 10 (red open squares), and ρ = 50 (green open circles), respectively.
    Fig. 3. Data collapse plot of (a) the average occupation number mk versus δc at the transient time t = 210, (b) the evolution of ratio of IPR to its steady state limit, It/I, versus t/ρν, with ν = 1 – δ being the dynamic exponent in the relaxation dynamics, at δ = 0.2 for network size L = 4000, and various densities ρ = 0.5 (purple open diamonds), ρ = 2 (blue open triangles), ρ = 10 (red open squares), and ρ = 50 (green open circles), respectively.
    δmk < kckcmk > kc
    δ > δc
    δ = δcρδck/(ln kmax)δc(ln kmax/ρ)δcρk1/δc/ln kmax
    δ < δc
    Table 1. The scaling relations of the crossover degree kc and the average degree occupation number mk w.r.t. the finite density ρ and the parameter δ.
    Guifeng Su, Xiaowen Li, Xiaobing Zhang, Yi Zhang. Finite density scaling laws of condensation phase transition in zero-range processes on scale-free networks[J]. Chinese Physics B, 2020, 29(8):
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