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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.

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.

2 Sep 2012: Phys Rev E Stat Nonlin Soft Matter Phys 80:041922.22. Ishikawa T, Locsei JT, Pedley TJ (2008) Development of coherent structures in concen-. ... Science 325:487–490. 43. Pedley TJ, Kessler JO (1992) Hydrodynamic phenomena in suspensions of

16 May 2012: Let Ti,(i = 1,2,3) denote a basis of su(2) with commutation relations [Ti,Tj] = ϵijkTk and TiT i := TiTjδij = 3412.

5 Sep 2012: Science 317:105–108. 52. Pedley TJ (2010) Collective behaviour of swimming micro-organisms.

15 Aug 2012: PERCOLATION ANDDISORDERED SYSTEMS. Georey GRIMMETT. 2PREFACEThis course aims to be a (nearly) self-contained account of part of the mathematicaltheory of percolation and related topics. The rst nine chapters summarise rigorousresults in percolation

2 Sep 2012: FL43CH26-Koch ARI 15 November 2010 14:32. Collective Hydrodynamics ofSwimming Microorganisms:Living FluidsDonald L. Koch1 and Ganesh Subramanian21 School of Chemical and Biomolecular Engineering, Cornell University, Ithaca,New York 14853; email:

2 Sep 2012: J Fluid Mech 669:167–177.21. Ishikawa T, Locsei JT, Pedley TJ (2010) Fluid particle diffusion in a semidilute suspension.

2 Sep 2012: Due to the linearity of the Stokes equations, theirtranslational and rotational velocities, vi and ωi, dependlinearly on all external forces and torques, Fj and Tj [12,18]:.

15 Aug 2012: PERCOLATION ANDDISORDERED SYSTEMSGeorey GRIMMETT. 2PREFACEThis course aims to be a (nearly) self-contained account of part of the mathematicaltheory of percolation and related topics. The rst nine chapters summarise rigorousresults in percolation

19 Jul 2012: #! /bin/sh # Guess values for system-dependent variables and create Makefiles. # Generated by GNU Autoconf 2.59 for OxbridgeKinetics 0.6. # # Report bugs to lester@hep.phy.cam.ac.uk. # # Copyright (C) 2003 Free Software Foundation, Inc. # This

2 Nov 2012: E. C. QUIGGIN MEMORIAL LECTURES 5. JOHN HINES. Old-Norse Sources for Gaelic History. DEPARTMENT OF ANGLO-SAXON, NORSE, AND CELTIC. UNIVERSITY OF CAMBRIDGE. Edmund Crosby Quiggin (1875-1920) was the first teacher of Celtic in the University of

2 Sep 2012: Magar V, Goto T, Pedley TJ (2003) Q J Mech Appl Math 56:65–91.35.

14 Oct 2012: equations, of which equation j has tj coefficients. The horizontal lines divide the groups of.

2 Sep 2012: CURRENT TOPICS IN PLANT RESEARCH. The sliding theory of cytoplasmic streaming: fifty yearsof progress. Teruo Shimmen. Received: 18 August 2006 / Accepted: 22 November 2006 / Published online: 25 January 2007! The Botanical Society of Japan and

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

2 Sep 2012: 52 predicts for a single receptor if IJ = TJ(1 - p).