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Three theorems in discrete random geometry
www.statslab.cam.ac.uk/~grg/papers/PS_2011_185-rev.pdf27 Jan 2012: The outcome is a decomposition ofγ into an ordered set of bridges with vertical displacements written T0 > T1 > > Tj. ... Therefore,. Z(x) 2. Ti<<T1T0>>Tj. j. k=i. ζxTk = 2. T =1. -
A R T I C L E Structure-based prediction ...
www-vendruscolo.ch.cam.ac.uk/sahakyan11jbnmr.pdf15 Jan 2012: A R T I C L E. Structure-based prediction of methyl chemical shifts in proteins. Aleksandr B. Sahakyan • Wim F. Vranken •. Andrea Cavalli • Michele Vendruscolo. Received: 18 March 2011 / Accepted: 17 May 2011 / Published online: 12 July 2011. -
The Isolation Time of Poisson Brownian Motions Yuval Peres∗ ...
www.statslab.cam.ac.uk/~ps422/isolation.pdf14 Mar 2012: 9. Define inductively. Tj1 = inf{m Tj 1 : i = 2,. ... E. κj=1. 1(x1 ξ1(Tj) U1Tj ). . By the independence of the motions of the nodes 1,. -
sieve.dvi
www.statslab.cam.ac.uk/~grg/papers/USsieve.pdf15 Aug 2012: Secondly, in (2.13) on page6, we assume further that tj < 12sj. ... The nal display on that page becomes1njI f1; 2; : : :;ngj 1n Xj: jRsj2n 1 nsj tj 3 XjR tjsj 3:AcknowledgementsThe author is grateful to Maury Bramson for taking an interest -
Mathematical Tripos Part III Lent Term 2012Advanced Quantum Field ...
www.damtp.cam.ac.uk/user/ho/aqft.pdf27 Jan 2012: Forcr = 0 show that det AN = N 1. If D(tj ) = det Aj show that as N we have. -
neessnmeiwseis.dvi
https://www.dpmms.cam.ac.uk/~md384/neessnmeiwseis.pdf27 Nov 2012: Part III Differential GeometryLecture Notes. Mihalis Dafermos. Contents. 1 Introduction 3. 1.1 From smooth surfaces to smooth manifolds. 31.2 What defines geometry? 51.3 Geometry, curvature, topology. 7. 1.3.1 Aside: Hyperbolic space and -
Minkowski dimension of Brownian motion with drift Philippe H. ...
www.statslab.cam.ac.uk/~ps422/minkowski.pdf3 Aug 2012: the ball B(f(tj),ε) is contained in B(f(ti), (2k1 1)ε). ... S(k) = {j : |ti tj| < 2ε and |f(ti) f(tj)| [2kε, 2k1ε)},. -
notes.dvi
www.statslab.cam.ac.uk/~grg/papers/USrednotes.pdf15 Aug 2012: PERCOLATION ANDDISORDERED SYSTEMSGeorey GRIMMETT. 2PREFACEThis course aims to be a (nearly) self-contained account of part of the mathematicaltheory of percolation and related topics. The rst nine chapters summarise rigorousresults in percolation -
https://www.hep.phy.cam.ac.uk/~lester/teaching/Computing2021/www.infer…
https://www.hep.phy.cam.ac.uk/~lester/teaching/Computing2021/www.inference.phy.cam.ac.uk/teaching/comput/C++/solutions/planet/Planet2.cc24 Sep 2012: // Planet2.cc // see also gnu20, gnu21 // usage: // Planet2 1300 0.03 25 | gnuplot -persist // This program requires the directory 'output' to exist, and // expects it to contain a file gnu0. #include iostream #include fstream #include cmath -
crit6.dvi
www.statslab.cam.ac.uk/~grg/papers/UScrit6.pdf15 Aug 2012: t0,x0,. ,xr1, tr) for some r 0 with xi Z2{O}, ti T, and tj 6= R for. ... iii) r = s 1, xi = yi for i r 1, tj = uj for j r, ys O and us = R.
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