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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.

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,

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

21 Feb 2023: 2022 European Mathematical SocietyPublished by EMS Press. J. Eur. Math. Soc. (Online first) DOI 10.4171/JEMS/1289. Matthew J. Colbrook Anders C. Hansen. The foundations of spectral computations via theSolvability Complexity Index hierarchy. Received

5 May 2020: Computational Projects. Lecture 6: Improving LU decomposition. http://www.maths.cam.ac.uk/undergrad/catam/part-ia-lectures. Dr Rob Jack, DAMTP. Recall. Suppose we want to solve Ax = b with. A =. 0 11 0. , b =. 23. <latexit

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.