Continuum Percolation
By I. Balberg. Encyclopedia of Complexity and Systems Science, 2009
647 citations recorded by the source corpus.
Subfields: Condensed Matter Physics, Materials Chemistry, Mathematical Physics
View Paper: https://www.semanticscholar.org/paper/15c9f294d8d1b820f7a30f9c96b2674dd67c6194
How researchers see this paper
The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.
In Condensed Matter Physics
- Scott Sheffield
- Wendelin Werner
- Eliran Subag
- Sertac Karaman
- Markus Heydenreich
- Mathew D. Penrose
- Terry Soo
- Peter Morters
In Materials Chemistry
- François Baccelli
- Matthias Schulte
- Günter Last
- Eliran Subag
- Sertac Karaman
- Markus Heydenreich
- Wendelin Werner
- Mathew D. Penrose
In Mathematical Physics
- Matthias Schulte
- Günter Last
- Mathew D. Penrose
- Jeffrey G. Andrews
- Scott Sheffield
- Wendelin Werner
- Martin Haenggi
- Daniel Hug
Citations in the corpus
- The topology of probability distributions on manifolds (2013, result): “There is a natural connection of the results in this paper with results in point processes, specifically random set models such as the Poisson-Boolean model [37].”
- Stochastic geometry and random graphs for the analysis and design of wireless networks (2009, background): “Gilbert’s original model has undergone many generalizations, and continuum percolation theory is now a rich mathematical fi eld, see [2], [35].”
- Scale-free percolation (2011, neutral): “A continuum analogue of long-range percolation, known as the random connection model, is described in [27].”
- Closing the Gap in the Capacity of Wireless Networks Via Percolation Theory (2007, background): “Percolation theory [9], [15] is a field of mathematics and statistical physics that provides models of phase transition phenomena that are observed in nature.”
- Sampling-based algorithms for optimal motion planning (2011, background): “In other words, for all λ > λc, there is a non-zero probability that the origin is in an infinite connected component of Gdisc∞ ( λ, 1); moreover, under these conditions, the graph has precisely one infinite connected component, almost surely (Meester and Roy 1996).”
- Gaussian Limts for Random Geometric Measures (2007, background): “1 Germ-grain models Germ-grain models are a fundamental model of random sets in stochastic geometry; see for example (9; 15; 26).”
- Conformal loop ensembles: the Markovian characterization and the loop-soup construction (2010, background): “Note that the standard arguments developed in the context of Mandelbrot percolation (see [23], [6]) can be easily adapted to the present setting in order to prove that c0 is subcritical, but not in the sense we have defined it.”
- CONNECTIVITY OF SOFT RANDOM GEOMETRIC GRAPHS (2013, background): “Soft random geometric graphs of this type are a finite-space version of the socalled random connection model of continuum percolation; see [11, 13], which describe further motivation, and see [11, Section 1.”
- Insertion and deletion tolerance of point processes (2010, background): “The Boolean continuum percolation model for point processes is defined as follows (see [19]).”
- Recurrence versus transience for weight-dependent random connection models (2019, methodology): “For further constructions, see Last and Ziesche [25] and Meester and Roy [28].”
- Random geometric complexes in the thermodynamic regime (2014, methodology): “We start with some definitions from percolation theory for the Boolean model on Poisson processes ([24]) needed for the proof of the Poisson central limit theorem.”
- Second-order properties and central limit theorems for geometric functionals of Boolean models (2013, background): “This is a fundamental model of stochastic geometry and continuum percolation with many applications in materials science and physics [3, 7, 17, 20, 28].”
- A parsimonious model of mobile partitioned networks with clustering (2009, background): “The region A l can be generated, for example, as the union of m random disks ofradius rl, and Ah its complement (cf. Figure 1). where: • Z (0) is an initial position in the torus; • Zx and Zy satisfies the following conditions: (4)”
- Poisson process Fock space representation, chaos expansion and covariance inequalities (2009, background): “In Section 5 we prove some results on covariances, including the following HarrisFKG inequality; see also [26], [4] (treating special Poisson processes) [43], and [9] for more general point processes.”