Convergence of Achlioptas Processes via Differential Equations with Unique Solutions
暂无分享,去创建一个
[1] B. Bollobás. The evolution of random graphs , 1984 .
[2] J. Norris,et al. Smoluchowski's coagulation equation: uniqueness, non-uniqueness and a hydrodynamic limit for the stochastic coalescent , 1998, math/9801145.
[3] Oliver Riordan,et al. Achlioptas processes are not always self-averaging. , 2011, Physical review. E, Statistical, nonlinear, and soft matter physics.
[4] Béla Bollobás,et al. Random Graphs , 1985 .
[5] S N Dorogovtsev,et al. Explosive percolation transition is actually continuous. , 2010, Physical review letters.
[6] Svante Janson,et al. Phase transitions for modified Erdős–Rényi processes , 2010, 1005.4494.
[7] Xuan Wang,et al. Bounded-Size Rules: The Barely Subcritical Regime , 2014, Comb. Probab. Comput..
[8] Svante Janson,et al. Random graphs , 2000, Wiley-Interscience series in discrete mathematics and optimization.
[9] Alan M. Frieze,et al. Avoiding a giant component , 2001, Random Struct. Algorithms.
[10] T. G. Seierstad. A central limit theorem via differential equations , 2009, 0906.4202.
[11] Svante Janson. Networking—Smoothly Does It , 2011, Science.
[12] Oliver Riordan,et al. Explosive Percolation Is Continuous , 2011, Science.
[13] D. Aldous. Deterministic and stochastic models for coalescence (aggregation and coagulation): a review of the mean-field theory for probabilists , 1999 .
[14] N. Wormald. The differential equation method for random graph processes and greedy algorithms , 1999 .
[15] Amarjit Budhiraja,et al. Bohman-Frieze processes at criticality and emergence of the giant component , 2011 .
[16] J. Spencer,et al. Explosive Percolation in Random Networks , 2009, Science.
[17] Oliver Riordan,et al. The evolution of subcritical Achlioptas processes , 2012, Random Struct. Algorithms.
[18] Michael Mitzenmacher,et al. Local cluster aggregation models of explosive percolation. , 2010, Physical review letters.
[19] Xuan Wang,et al. Aggregation models with limited choice and the multiplicative coalescent , 2015, Random Struct. Algorithms.
[20] Eric J Friedman,et al. Construction and analysis of random networks with explosive percolation. , 2009, Physical review letters.
[21] O. Riordan,et al. Achlioptas process phase transitions are continuous , 2011, 1102.5306.
[22] Finite-size scaling theory for explosive percolation transitions. , 2010, Physical review. E, Statistical, nonlinear, and soft matter physics.
[23] Witold Hurewicz,et al. Lectures on Ordinary Differential Equations , 1959 .
[24] Tom Bohman,et al. Creating a Giant Component , 2006, Comb. Probab. Comput..
[25] Svante Janson,et al. Random graphs , 2000, ZOR Methods Model. Oper. Res..
[26] Santo Fortunato,et al. Explosive percolation: a numerical analysis. , 2009, Physical review. E, Statistical, nonlinear, and soft matter physics.
[27] Eli Upfal,et al. Balanced Allocations , 1999, SIAM J. Comput..
[28] N. Wormald. Differential Equations for Random Processes and Random Graphs , 1995 .
[29] Joel H. Spencer,et al. Birth control for giants , 2007, Comb..
[30] Joel H. Spencer,et al. The Bohman‐Frieze process near criticality , 2011, Random Struct. Algorithms.
[31] P. Erdos,et al. On the evolution of random graphs , 1984 .
[32] A. Gut. Probability: A Graduate Course , 2005 .
[33] B. Bollobás,et al. The phase transition in inhomogeneous random graphs , 2007 .
[34] Béla Bollobás,et al. Random Graphs and Branching Processes , 2008 .
[35] Robert M Ziff,et al. Explosive growth in biased dynamic percolation on two-dimensional regular lattice networks. , 2009, Physical review letters.