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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)},. -
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. -
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 -
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. -
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 -
Cambridge University Reporter, Friday, 16 December 2011
https://www.reporter.admin.cam.ac.uk/reporter/2011-12/special/05/05.pdf8 Feb 2012: University Officers, Michaelmas Term 2011 ('Officers Number', Part I) -
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 -
Department of Pure Mathematics and Mathematical StatisticsUniversity…
https://www.dpmms.cam.ac.uk/~tkc/GeometryandGroups/GeometryandGroups.pdf27 Nov 2012: The real numbers tj can be written as tj = kj t′j with kj Zand 0 6 t′j < 1. -
Fou3.dvi
https://www.dpmms.cam.ac.uk/~twk/Fou3.pdf24 Jul 2012: tm) =m. j=1. Kn(tj),. then we have the following results. -
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 -
FENLAND FIELD TRIP
https://www.geog.cam.ac.uk/files/research/projects/ribago/ribago2010fieldtrip.pdf8 Feb 2012: 1848-1978 A.D. Journal of Ecology 68, 229-249 Lock, JM, Friday, LE & Bennett, TJ (1997) ‘The management of the fen’, in LE Friday (ed.). -
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. -
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. -
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,. -
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 -
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. -
10-grg.dvi
www.statslab.cam.ac.uk/~grg/books/hammfest/10-grg.pdf15 Aug 2012: n,(c) if ti = tj , then (ti, zi) / (tj , zj ) in {ti} Zd, for 0 i < j n. -
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 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: -
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.
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