Search

21 Mar 2012: The new drug is untested and has an unknown probability of success θ,which the doctor believes to be uniformly distributed over [0, 1]. ... For example, suppose p = 0.6 and 6 trials with the new drug have givens = f = 3.

15 Aug 2012: This is certainly achieved if the earliest jHjk such sr eachstrikes a new integer of H, i.e., an integer struck by no smaller sr (here and laterwe sometimes use real

15 Aug 2012: R. (1989), Percolation, Springer, New York.7. Grimmett, G. R. (1994), Potts models and random-cluster processes with many-bodyinteractions, Journal of Statistical Physics 75, 67–121.

15 Aug 2012: Stochastic Processes and their Applications 26 (1987), 1–30. 9. Janson, S., New versions of Suen’s correlation inequality, Random Structures and Algorithms.

15 Aug 2012: For example, the critical probability of a percolationprocess cannot increase if new edges are added to the lattice. ... Such monotonicity, when true, is usually easy to prove. Strict monotonicity, onthe other hand, presents new difficulties.

15 Aug 2012: Their solutions require a mixture of new ideas, from analysis, geometry, anddiscrete mathematics.

15 Aug 2012: phase diagram of a modied epidemic model in which new susceptiblesare born at some positive rate. ... M. (1985). Interacting Particle Systems. Springer-Verlag, New York.Menshikov, M. V. (1986).

23 Jul 2012: Thelast model is especially challenging because it is non-ferromagnetic, and thus givesrise to new problems of importance and difficulty. ... There are many new complications and some of the basic questions remainunanswered, at least in part.

15 Aug 2012: solve.• Their solutions require a mixture of new ideas, from analysis, geometry,.

15 Aug 2012: We continue similarly, at each stage picking anew trifurcation tk Λ and a new vertex yk Λ.

15 Aug 2012: Thus, from every pair Ci, Cj ofdistinct components, we obtain new elements F ′ of Fs1 by adding an edge joiningCi to Cj. ... their Applications 59 (1995), 267–275. 13. Janson, S., Luczak, T., Ruciński, A., Random Graphs, Wiley, New York, 2000.14.

15 Aug 2012: N ). We writeg = (gki : 1 i N ) for the associated function given by (2.12)–(2.14)subject to the new ordering, and C = g1(A). ... j1, j1,. , N}, and we construct a continuous increasing function g as abovebut subject to the new ordering.

15 Aug 2012: The principal new technique is aform of Russo's formula for random-cluster models reported by Bezuidenhout, Grimmett, andKesten.

15 Aug 2012: In this new network there are jeB(n)j parallelconnections between @B(n) and @B(n1), each of which has (for n M = M(Z))a resistance exceeding c= logn (by

2 Jul 2012: There has been a great deal of interest and activity in percolation theorysince the two Saint-Flour courses, [76, 111], of 1984 and 1996 reprinted inthis new edition. ... Press, New York, 1990,pp. 167–190. 91. O. Häggström, Uniqueness in

20 Dec 2012: We discuss these conditions in detail in Sections 3.2 and 3.3 respectively andcompare both the original and the new bounds to demonstrate the marked improvement. ... Our improved bounds are based on new versions of Markov’s inequality that hold for

15 Aug 2012: New difficulties arise through the presenceof orientations on the edges of the underlying lattice, and new ideas are neededto overcome these problems. ... 8, Springer, Berlin–Heidelberg–New York, 1987, pp. 13–20. 2. Aizenman, M., Newman, C.

15 Aug 2012: Having constructed tm1,we define tm = tm(X, X) by adding to tm1 a new edge 〈ξim , ξm〉 where 1 im < mand ξm ( X{ξ1, ξ2,. ,

15 Aug 2012: The percolation model contains a maxi-mum of (statistical) independence, and has proved a superb testing ground for new. ... Percolation theory has earned a reputation as a source of hard problems which areeasy to state and whose solutions require new

11 Apr 2012: U. In the latter case, we may remove U together with the previous DV stepto obtain a new admissible Λ-path from 0 to x of shorter length than π , a