Percolation - Measure - Probability

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SUMMARY

The discussion focuses on the mathematical framework of percolation theory within the context of the set $\Omega = \{0,1\}^{\mathbb{Z}^{2}}$. It establishes that the class of cylinders, denoted as $C$, forms an algebra and explores the $\sigma$-algebra generated by $C$, represented as $\mathbb{F}=\sigma(C)$. Key events are defined, including the infinite cluster of the origin, the existence of an infinite cluster system, positive density of the origin's cluster, and the existence of at least two distinct infinite clusters.

PREREQUISITES
  • Understanding of percolation theory
  • Familiarity with $\sigma$-algebras in probability theory
  • Knowledge of cluster points and their properties in $\mathbb{Z}^{2}$
  • Basic concepts of algebraic structures in set theory
NEXT STEPS
  • Study the properties of $\sigma$-algebras in probability theory
  • Explore advanced topics in percolation theory, focusing on infinite clusters
  • Learn about the implications of cluster density in percolation models
  • Investigate the relationship between cylinders and algebraic structures in set theory
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Mathematicians, statisticians, and researchers in probability theory, particularly those interested in percolation models and their applications in various fields such as physics and network theory.

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In $\Omega = \{0,1\}^{\mathbb{Z}^{2}}$, consider the class $C$ of cylinders. Show that $C$ is algebra. At $w\in \Omega$, we call cluster point $x$ all points $z\in \mathbb{Z}^{2}$ that can be attained from $x$ by a path that only passes by open dots. In the $\sigma$-algebra generated by $C, \mathbb{F}=\sigma(C)$, express the following events explicitly:

1 - {The cluster of the origin is infinite}

2 - {Exist in an infinite cluster system}

3 - {The cluster of the origin has positive density}

4 - {exist at least two infinite clusters (distinct)}
 
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$\Omega = \{0,1\}^{\mathbb{Z}^{2}}$ is the set of open and closed $\mathbb{Z}^{2}$

$\Omega_{\wedge} = \{0,1\}^{\wedge}, \forall \wedge \subset \mathbb{Z^{2}}$ finite.

$C:=$Cylinders (That is, local events that depend on a finite number of sites);

$\Pi_{\wedge}:\Omega \rightarrow \Omega_{\wedge}$ defined by $\Pi_{\wedge}(w)=$coincides with $w$ in $\wedge;$

$C_{\wedge}:=\Pi_{\wedge}^{-1}(P(\Omega_{\wedge}))$, where $P(\Omega_{\wedge})$ is the power set of $\Omega_{\wedge};$

In $\Omega = \{0,1\}^{\mathbb{Z}^{2}}$, consider the class $C$ of cylinders. Show that $C$ is algebra. At $w\in \Omega$, we call cluster point $x$ all points $z\in \mathbb{Z}^{2}$ that can be attained from $x$ by a path that only passes by open dots. In the $\sigma$-algebra generated by $C, \mathbb{F}=\sigma(C)$, express the following events explicitly:

1 - {The cluster of the origin is infinite}

2 - {Exist in an infinite cluster system}

3 - {The cluster of the origin has positive density}

4 - {exist at least two infinite clusters (distinct)}
 

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