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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. -
The Mechanics and Statistics of Active Matter
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/Ramaswamy10.pdf2 Sep 2012: The Mechanics and Statisticsof Active Matter. Sriram Ramaswamy. Centre for Condensed Matter Theory, Department of. Physics, Indian Institute of Science, Bangalore 560012,. India and CMTU, JNCASR, Bangalore 560064, India;. email: -
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,. -
Stratosphere‐Troposphere Exchange
www.damtp.cam.ac.uk/user/mem/papers/STE/holton-etal-strat-trop-revsgeoph95.pdf22 Aug 2012: whereas the response to a force at a latitude equator- ward of that given by the right-hand side of (9) appears primarily as an acceleration, O tJ/Ot, rather than -
Solitons from Geometry Maciej Dunajski Department of Applied…
www.damtp.cam.ac.uk/user/md327/solitons_france_2012.pdf5 Dec 2012: γ+ su(2) self–dual YM on (M,g) Skyrmion on M/SO(2). A = (1/2)εijkγij tk, where [ti,tj] = εijktk.AH, Taub–NUT, CP2 are SO(3) invariant. -
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 -
pnas201206839 17424..17429
https://www2.mrc-lmb.cam.ac.uk/groups/rlw/download/publications/23045692.pdf21 Nov 2012: midbody and function in cytokinesis. EMBO J 26(19):4215–4227.6. Lindås AC, Karlsson EA, Lindgren MT, Ettema TJ, Bernander R (2008) A unique cell. -
pnas201204185 12788..12793
www.memlab.psychol.cam.ac.uk/pubs/Fornito2012%20PNAS.pdf1 Aug 2012: Competitive and cooperative dynamics of large-scalebrain functional networks supporting recollectionAlex Fornitoa,b,c,1, Ben J. Harrisona, Andrew Zaleskya, and Jon S. Simonsd,e. aMelbourne Neuropsychiatry Centre, Department of Psychiatry, University -
Physics of chemoreception
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/BergPurcell77.pdf2 Sep 2012: 52 predicts for a single receptor if IJ = TJ(1 - p). -
pcbi.1002169 1..9
www-vendruscolo.ch.cam.ac.uk/fitzpatrick11pcb.pdf15 Jan 2012: 18. Linding R, Russell RB, Neduva V, Gibson TJ (2003) GlobPlot: Exploringprotein sequences for globularity and disorder. -
Old Norse Sources for Gaelic History
https://www.asnc.cam.ac.uk/publications/Quiggin/ECQ%20Vol%205%202002%20Hines.pdf2 Nov 2012: E. C. QUIGGIN MEMORIAL LECTURES 5. JOHN HINES. Old-Norse Sources for Gaelic History. DEPARTMENT OF ANGLO-SAXON, NORSE, AND CELTIC. UNIVERSITY OF CAMBRIDGE. Edmund Crosby Quiggin (1875-1920) was the first teacher of Celtic in the University of -
notes.dvi
www.statslab.cam.ac.uk/~grg/papers/USstflour.pdf15 Aug 2012: PERCOLATION ANDDISORDERED SYSTEMS. Georey 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 -
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 -
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)},. -
Microfluidics of cytoplasmic streaming and itsimplications for…
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/GoldsteinTuvalvandeMeent08.pdf2 Sep 2012: Magar V, Goto T, Pedley TJ (2003) Q J Mech Appl Math 56:65–91.35. -
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. -
Male-killing Wolbachia do not protect Drosophila bifasciata against…
www.jiggins.gen.cam.ac.uk/pdfs/longdon2012.pdf19 Jan 2012: Plos One 2010, 5. 24. Himler AG, Adachi-Hagimori T, Bergen JE, Kozuch A, Kelly SE, Tabashnik BE,Chiel E, Duckworth VE, Dennehy TJ, Zchori-Fein E, Hunter MS: Rapid spreadof -
Light–matter interaction in a microcavity-controlled…
www-g.eng.cam.ac.uk/nms/publications/pdf/Michael_NatComm2012.pdf20 Jun 2012: Farmer (IBM TJ Watson Research Center) for atomic layer deposition, R. ... Ferlito (CSS, IBM TJ Watson Research Center) for Ag mirror deposition and B.A.Ek (IBM TJ Watson Research Center) for expert technical assistance. -
lectures2012.dvi
www.damtp.cam.ac.uk/user/phh/mathbio/lectures2012.pdf6 Jun 2012: Cop. yrig. ht. 201. 2 U. nive. rsity. of C. ambr. idge. Not. to b. e qu. oted. or. repr. oduc. ed w. ithou. t per. mis. sion. Part II Mathematical Biology Lent Term 2012. lecturer: Professor Peter Haynes (phh@damtp.cam.ac.uk). May 31, 2012. These
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