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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)},. -
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,. -
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) -
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. -
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 -
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:
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