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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

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

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

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.

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.

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

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

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]:.

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:

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