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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:

3 Jul 2008: Adiabatic limit and the slow motion of vortices in a. Chern-Simons-Schroedinger system. Sophia Demoulini and David StuartCentre for Mathematical Sciences, Wilberforce Road, Cambridge, CB3 OWB, England. email:sd290@cam.ac.uk, dmas2@cam.ac.uk.

22 Jul 2010: J. Fluid Mech. (1978), wol. 89, part 4 , p p. 609-646. Printed i n Great Britain 609. An exact theory of nonlinear waves on a Lagrangian-mean flow. By D. G. A N D R E W S U.K. Universities’ Atmospheric Modelling Group,. Reading, Berkshire,

14 Nov 2004: DAMTP 2004/NA05. The NEWUOA software for unconstrained. optimization without derivatives1. M.J.D. Powell. Abstract: The NEWUOA software seeks the least value of a function F (x),xRn, when F (x) can be calculated for any vector of variables x. The

30 May 2018: ,. where tj = 1 0.5(sin(j) i cos(j)) for j 4.

12 Jul 2017: Kim TJ, Hidrovo C (2012) Pressure and partial wetting effects on superhydrophobicfriction reduction in microchannel flow.

21 Nov 2007: k)tj of the expression. 2Λ(k)t =m. j=1 µ(k)tj (y. (k)j x̂) (y(k).

23 Nov 2023: Group Theory Lecture Notes. Hugh Osborn. latest update: November 23, 2023. Based on part III lectures Symmetries and Groups, Michaelmas Term 2008, revised andextended at various times subsequently. Books. Books developing group theory by physicists

1 Dec 2023: Journal of Glaciology. Article. Present address: Alfred Wegener Institute,Helmholtz Centre for Polar and MarineResearch, Bremerhaven, Germany. †Present address: Byrd Polar & ClimateResearch Center, The Ohio State University,1090 Carmack Rd,

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.