Search

3 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)},.

27 Jan 2012: Forcr = 0 show that det AN = N 1. If D(tj ) = det Aj show that as N we have.

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

20 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.

1 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

8 Feb 2012: University Officers, Michaelmas Term 2011 ('Officers Number', Part I)

27 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

27 Nov 2012: The real numbers tj can be written as tj = kj t′j with kj Zand 0 6 t′j < 1.

24 Jul 2012: tm) =m. j=1. Kn(tj),. then we have the following results.

24 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

8 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.).

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.

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.