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The 1-2 model
www.statslab.cam.ac.uk/~grg/papers/conm14020.pdf18 Aug 2017: lattice. This last problemmay be solved using the Pfaffian representation of Kasteleyn [15], Fisher [5], andTemperley and Fisher [24]. ... Inform.Theory 54 (2008), no. 5, 2179–2195, DOI 10.1109/TIT.2008.920245. MR2450856. [24] H. -
ON BAYESIAN INFERENCE FOR SOME STATISTICAL INVERSEPROBLEMS WITH…
www.statslab.cam.ac.uk/~nickl/Site/__files/bnews.pdf6 Nov 2017: This letter (Bernoulli News, Vol. 24 (2), 2017) summarizes key ideas from the Ethel Newboldprize lecture. -
SELF-AVOIDING WALKS AND AMENABILITY GEOFFREY R. GRIMMETT AND…
www.statslab.cam.ac.uk/~grg/papers/new10.pdf3 Jul 2017: 23–38.[24] J. M. Hammersley and D. J. A. Welsh, Further results on the rate of convergence to the. ... 5,. 2002, available at http://arxiv.org/abs/math/0212142. 24 GEOFFREY R. GRIMMETT AND ZHONGYANG LI. -
0. Statistics 1B Statistics 1B 1 (1–1) 0. Lecture ...
www.statslab.cam.ac.uk/Dept/People/djsteaching/S1B-17-01-intro-prob.pdf18 Jan 2017: barplot( dbinom(0:10, 10, 1/6), names.arg=0:10,. xlab="Number of sixes in 10 throws" ). Lecture 1. Introduction and probability review 24 (1–1). 1. Introduction and probability -
0. Statistics 1B Statistics 1B 1 (1–1) 0. Lecture ...
www.statslab.cam.ac.uk/Dept/People/djsteaching/S1B-17-01-intro-prob-4.pdf17 Jan 2017: barplot( dbinom(0:10, 10, 1/6), names.arg=0:10,. xlab="Number of sixes in 10 throws" ). Lecture 1. Introduction and probability review 24 (1–1). 1. Introduction and probability -
Convergence of the SAW on random quadrangulations to SLE8/3 on…
www.statslab.cam.ac.uk/~jpm205/slides/saw_convergence_paris_january_2017.pdf22 Jan 2017: Jason Miller (Cambridge) Convergence of the SAW on ’s to SLE(8/3) January 24, 2017 6 / 26. ... Jason Miller (Cambridge) Convergence of the SAW on ’s to SLE(8/3) January 24, 2017 7 / 26. -
Strong law of large numbers for the capacity of ...
www.statslab.cam.ac.uk/~ps422/wiener7.pdf22 Dec 2017: Then using again that ‖βs β(τδi )‖ δ, for all s [τδi ,τδi1], and (3.24) we get for all δ 1,. ... 24. We consider two independent Brownian motions (βt, t 0) and (β̃t, t 0) starting respectivelyfrom 0 and z, and denote their corresponding -
Connective constants and height functions for Cayley graphs
www.statslab.cam.ac.uk/~grg/papers/tran7166.pdf18 Aug 2017: Such harmonic functions do not appear to contribute to thediscussion of the Liouville property (see, for example, [24, Defn 2.1.10]), since boththeir positive and negative parts are unbounded. -
BriefingPukelsheimGrimmettFinalVersion-4
www.statslab.cam.ac.uk/~grg/papers/BriefingPukelsheimGrimmettFinalVersion-4.pdf10 Feb 2017: Netherlands 17 235 349 392 421 427.3 32 531 580 26 6 Belgium 11 289 853 282 962 419.7 24 455 719 21 3 Greece 10 793 526 273 ... 297 419.03 24 447 895 21 3 Czech Republic 10 445 783 266 466 418.6 23 442 225 21 2 Portugal 10 341 330 264 404 418.4 23 -
CRITICAL SURFACE OF THE 1-2 MODEL GEOFFREY R. GRIMMETT ...
www.statslab.cam.ac.uk/~grg/papers/12-final-revised.pdf17 Feb 2017: 24 GEOFFREY R. GRIMMETT AND ZHONGYANG LI. To H we assign a clockwise odd orientation as in Figure 5.3: the figure shows aclockwise odd orientation of H1,, embedded in a ... 7] and [24]. We now construct the modified Kasteleyn matrix K1(z,w) of H1, by
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