2 edition of **First-passage percolation on the square lattice** found in the catalog.

First-passage percolation on the square lattice

R. T. Smythe

- 262 Want to read
- 16 Currently reading

Published
**1978** by Springer-Verlag in Berlin, New York .

Written in English

- Limit theorems (Probability theory),
- Matrices.,
- Renewal theory.

**Edition Notes**

Other titles | Percolation on the square lattice. |

Statement | R.T. Smythe, John C. Wierman. |

Series | Lecture notes in mathematics -- 671, Lecture notes in mathematics (Springer-Verlag) -- 671. |

Contributions | Wierman, John C., 1949- |

Classifications | |
---|---|

LC Classifications | QA3 .L28 no. 671, QA273.67 .L28 no. 671 |

The Physical Object | |

Pagination | viii, 196 p. ; |

Number of Pages | 196 |

ID Numbers | |

Open Library | OL18024032M |

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First-Passage Percolation on the Square First-passage percolation on the square lattice book (Lecture Notes in Mathematics) th Edition by Robert T.

Smythe (Author), John C. Wierman (Contributor). First-Passage Percolation on the Square Lattice It seems that you're in USA. We have a dedicated First-Passage Percolation on the Square Lattice. Authors: Smythe, R.T., Wierman, J.C Other percolation models on the square lattice.

Pages Smythe, R. (et al.) Preview. First-Passage Percolation on the Square Lattice. Authors (view affiliations) R. Smythe; John C. Wierman Convergence First-passage percolation on the square lattice book the first-passage processes. Smythe, John C. Wierman Route length and the height process.

Smythe, John C. Wierman. Pages Other percolation models on the square lattice. Smythe, John C. First-Passage Percolation on the Square Lattice | R.T. Smythe, J.C. Wierman | download | B–OK.

Download books for free. Find books. First-passage percolation on the square lattice. I In First-passage percolation on the square lattice book 2 we verify, in a slightly altered form, a conjecture of Hammersley and Welsh to the effect that if the underlying distribution has an atom First-passage percolation on the square lattice book zero of size greater than C, the critical percolation probability, then jL = 0.

Let aon be the first-passage from (0,0) to (n,0). Hammersley and Welsh. Get this from a library. First-passage percolation on the square lattice. [R T Smythe; John C Wierman].

First-passage percolation on the square lattice. Preliminaries.- Bernoulli percolation.- Definition of the basic processes and the existence of routes.- Convergence of the first-passage processes.- Renewal theory for percolation processes.- The time constant.- Route length and the height process.- Other percolation models on.

Preliminaries --Bernoulli percolation --Definition of the basic processes and the existence of routes --Convergence of the first-passage processes --Renewal theory for percolation processes --The time constant --Route length and the height process --Other percolation models on the square lattice --Conjectures and open problems.

First-passage percolation on the square lattice, II The previous results of this section point out a difference between the cylinder and unrestricted first-passage times.

Hammersley and Welsh () employed the cylinder restriction to gain independence in the processes. The theorems. Let R(0;r) = fx: kxk rgbe the square with radius r centered at 0.

Recall that p c = 1=2 is the critical value for bond percolation on the two-dimensional lattice. For this and other facts we use about percolation, see Grimmett’s book [7]. Our rst result gives an upper bound on C 0(t). Theorem 1. For any >0 the probability First-passage percolation on the square lattice book 0(t) R(0;n(p.

First-passage First-passage percolation on the square lattice book on the square lattice. III p as in Hammersley and Welsh (). They proved ((), pp.

) that if U(A) =0 for some A >0 and pt'(0) exists, then () lim (NM/n) = L'(0) in probability, where 0 = a, b, s or t. Our proof of the stronger. Cite this chapter as: Smythe R.T., Wierman J.C. () Other percolation models on the square lattice.

In: First-Passage Percolation on the Square by: 2. The principal results of this paper concern the asymptotic behavior of the number of arcs in the optimal routes of first-passage percolation processes on the square lattice.

Assuming that the underlying distribution has an atom at zero less than λ –1, where λ is the connectivity constant, L p and (in some cases) almost sure convergence theorems are proved for the normalized route length by: Time constant of first-passage percolation on the square lattice proof of Theoremwhich simply tries to replace lim sup with lim inf, is more difficult.

The condition involving U in these theorems ensures that all other d.f.'s have finite means. It is a technical convenience, and can be weakened. In rst{passage percolation, introduced by Hammersley and Welsh [3], each edge is open, and associated with a random variable, representing the time for the uid to pass the bond.

First-passage percolation We will study the time constant for rst-passage percolation on the graph given by the square lattice. The vertices are the points (x;y. Smythe R.T., Wierman J.C. () Convergence of the first-passage processes. In: First-Passage Percolation on the Square Lattice.

Lecture Notes in Mathematics, vol Author: R. Smythe, John C. Wierman. The most famous model of first passage percolation is on the lattice. One of its most notorious questions is "What does a ball of large radius look like?".

This question was raised in the original paper of Hammersley and Welsh in and gave rise to the Cox-Durrett limit shape theorem in The time constant of first-passage percolation on the square lattice, Adv. Appl. Prob. 12, – zbMATH CrossRef Google Scholar [7] J.T.

Cox and R. Durrett ().Cited by: Percolation probabilities on the square lattice But E, E, are covariant and by symmetry P (E i)= P(E2). Hence it is enough to show that P (E,)3 (1- J(1- 7)) 2. But (by drawing a picture) E, occurs if, for some i, P, is open and F, is joined to U2 by an open path in by: for the square lattice ℤ 2 in two dimensions, p c = 12 for bond percolation, a fact which was an open question for more than 20 years and was finally resolved by.

Part of the Progress in Probability book series (PRPR, volume 54) First-passage percolation was introduced by Hammersley and Welsh in (see [13]), partly as a Cited by: Book review Open archive First-passage percolation on the square lattice: R. Smythe and J. Wierman, Springer-Verlag, Berlin/New York,pp.

Gian-Carlo Rota. Consider (independent) first-passage percolation on the sites of the triangular lattice T embedded in C. Denote the passage time of the site v in T by t (v), and assume that P (t (v) = 0) = P (t (v) = 1) = 1 ∕ 2.

Denote by b 0, n the passage time from 0 to the halfplane {v ∈ T: Re (v) ≥ n}, and by T (0, n u) the passage time from 0 to the Cited by: 7. For square contingency tables with ordered categories, Tomizawa () considered the polynomial diagonals-parameter symmetry (PDPS) model.

The present paper proposes the incomplete PDPS model which has the structure of PDPS for the partial cells of off-diagonal cells except a specified pair of cells and, in the table. The percolation threshold is a mathematical concept in percolation theory that describes the formation of long-range connectivity in random systems.

Below the threshold a giant connected component does not exist; while above it, there exists a giant component of the order of system size. We consider a model of long‐range first‐passage percolation on the d‐dimensional square lattice ℤd in which any two distinct vertices x,y ∊ ℤ d are connected by an edge having exponentially distributed passage time with mean ‖x–y‖ α+o(1), where α > 0 is a fixed parameter and ‖‖ is the l 1 –norm on ℤ analyze the asymptotic growth rate of the set ß t, which Cited by: 5.

LONG-RANGE FIRST-PASSAGE PERCOLATION 3 exhibits phase transition even in one dimension, it also displays discontinuous transition of percolation density for = 2 in one dimension as varies.

We refer the readers to [1,33,42,43] for more details about these works. Later, Benjamini and Berger [4] have proposed LRP onCited by: 5. Smythe RT, Wierman J ().

First-passage percolation on the square lattice, III. Advances in Applied Probability. Wierman JC (). On critical probabilities in percolation theory.

Journal of Mathematical Physics. 19(9). Smythe RT, Wierman J (). First passage percolation on the square lattice, II. Advances in. Conformally invariant processes in the plane.

percolation on the triangular lattice at critical probability, and uniform spanning trees were proved to converge in the scaling limit to SLE κ.

VARIATIONAL FORMULA FOR THE TIME-CONSTANT OF FIRST-PASSAGE PERCOLATION ARJUN KRISHNAN Abstract. We consider rst-passage percolation with positive, stationary-ergodic weights on the square lattice Zd.

Let T(x) be the rst-passage time from the origin to a point x in Zd. The convergence of the scaled rst-passage time T([nx])=n toCited by: 8. Chapter 11 is devoted to percolation in two dimensions, where the technique of planar duality leads to the famous exact calculation that $\pc =\half$ for bond percolation on $\zz^2$.

The book terminates with two chapters of pencil sketches of related random processes, including continuum percolation, first-passage percolation, random electrical. examples of the wide applicability of this theory, as well as percolation (e.g., in porous media) itself [7].

Although easily deﬁned, percolation presents theoretical and computational diﬃculties. For instance, the percolation threshold for the site problem on a simple square lattice is not known Size: KB.

In this paper we consider first passage percolation on the square lattice \(\mathbb{Z}^d\) with passage times that are independent and have bounded \(p^{th}\) moment for some \(p > 6(1+d),\) but not necessarily identically distributed.

For integer \(n \geq 1,\) let \(T(0,n)\) be the minimum time needed to reach the point \((n,\mathbf{0})\) from the by: 4. 2 What is Percolation. DRAFT [] xy Figure A sketch of the structure of a two-dimensional porous stone.

The lines indicate the open edges; closed edges have been omitted. On immersion of the stone in water, vertex x will be wetted by the invasion of water, but vertex y will remain dry. When can such inﬁnite clusters exist. Percolation.

Kesten's most famous work in this area is his proof that the critical probability of bond percolation on the square lattice equals 1/2. He followed this with a systematic study of percolation in two dimensions, reported in his book Percolation Theory for mater: Cornell University.

[13] Smythe, R. and Wierman, J. () First-Passage Percolation on the Square Lattice Springer Lecture Notes in MathematicsSpringer-Verlag, Berlin.

[14] Sykes, M. and Essam, J. () Exact critical percolation probabilities for the site and bond problems in two dimensions, J. Math. Phys. 5, – Cited by: We consider the first passage percolation model on the square lattice.

In this model, $\{t(e): e{an edge of}{\bf Z}^2 \}$ is an independent identically. First Passage Percolation on the Square Lattice. Lecture Notes in Math. Springer, Berlin.

Mathematical Reviews (MathSciNet): MR Law of large numbers for critical first-passage percolation on the triangular lattice Yao, Chang-Long, Electronic Communications in Probability, ;Cited by: We consider first-passage percolation on the two-dimensional triangular lattice T.

Each site v ∈ T is assigned independently a passage time of either 0 or 1 with probability 1 ∕ 2. Denote by B + (0, n) the upper half-disk with radius n centered at 0, and by c n + the first-passage time in B + (0, n) from 0 to the half-circular boundary of B Cited by: 1.

Multiple phase transitions in long range rst-passage percolation on square lattice Shirshendu Chatterjee Courant Institute of Mathematical Sciences, NYU Work in progress with Partha Dey J S.

Chatterjee Long range First-passage Percolation. Examples of percolation in a sentence, how to use it. examples: Long-range percolation is a natural model of some social networks, in which the.

Manfred Schroeder touches on the topic of percolation download pdf number of times in his encyclopaedic book on fractals (Schroeder, M. (). Fractals, Chaos, Power Laws: Minutes from an Infinite Paradise. W H Freeman & Company.). Percolation has numerous practical applications, the most interesting of which (from my perspective) is the flow of hot water through [ ].One of the simplest realizations of DP is bond directed model is ebook directed variant of ordinary (isotropic) percolation and can be introduced as follows.

The figure shows a tilted square lattice with bonds connecting neighboring sites.