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15 Jan 2012: 18. Linding R, Russell RB, Neduva V, Gibson TJ (2003) GlobPlot: Exploringprotein sequences for globularity and disorder.

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,.

19 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

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.

15 Aug 2012: n,(c) if ti = tj , then (ti, zi) / (tj , zj ) in {ti} Zd, for 0 i < j n.

15 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.

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:

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.

6 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

15 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.