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31 - 37 of 37 search results for tj KaKaotalk:PC53 where 0 match all words and 37 match some words.

  1. Results that match 1 of 2 words

  2. pnas201206839 17424..17429

    https://www2.mrc-lmb.cam.ac.uk/groups/rlw/download/publications/23045692.pdf
    21 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.

  3. sieve.dvi

    www.statslab.cam.ac.uk/~grg/papers/USsieve.pdf
    15 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

  4. Solitons from Geometry Maciej Dunajski Department of Applied…

    www.damtp.cam.ac.uk/user/md327/solitons_france_2012.pdf
    5 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.

  5. Stratosphere&hyphen;Troposphere Exchange

    www.damtp.cam.ac.uk/user/mem/papers/STE/holton-etal-strat-trop-revsgeoph95.pdf
    22 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

  6. The Isolation Time of Poisson Brownian Motions Yuval Peres∗ ...

    www.statslab.cam.ac.uk/~ps422/isolation.pdf
    14 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,.

  7. The Mechanics and Statistics of Active Matter

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/FDSE/Ramaswamy10.pdf
    2 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:

  8. Three theorems in discrete random geometry

    www.statslab.cam.ac.uk/~grg/papers/PS_2011_185-rev.pdf
    27 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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