Search

16 May 2024: P Le Sidaner, PA Loboda, HE Mason, NJ Mason, C Mendoza, G Mulas, TJ Millar, LA Nunez, VI Perevalov, N Piskunov, Y Ralchenko, G Rixon, LS Rothman, E Roueff, TA Ryabchikova,

16 May 2024: BC Allanach, TJ Khoo, K Sakurai. – Journal of High Energy Physics.

1 Dec 2021: 0/34. The finite-dimensional case. du. dt= Au, A Cnn, u(0) = u0 Cn u(t) = exp(tA)u0 =. j=0. tj. j!Aju0. E.g., if A = PDP1, D =

6 Jul 2011: 1. Pedley TJ, Kessler JO (1992) Hydrodynamic phenomena in suspensions of swimmingmicroorganisms.

7 Jan 2004: n̂m̂. j=1. sj zj z. Tj = Z. SZ+ T , (5.1). ... 2 zn̂m̂ zTn̂m̂. sn̂m̂ (eTt zn̂m̂)2. =n̂m̂1. j=1. sj zj zTj =. n̂m̂1. j=1. sj zj z. Tj. (5.9). We see that is the sum of the matrix

28 Oct 2006: This. isa. super. vis. or’. sco. py. ofth. enote. s.It. isnot. tobe. dis. trib. ute. dto. studen. ts. Natural Sciences Tripos: IB Mathematical Methods I. Contents. 0 Introduction i. 0.1 Schedule. i. 0.2 Books. ii. 0.3 Lectures. ii. 0.4 Printed

13 Jul 2009: With a streamfunction tj = r1 “f(0), th’ is no-slip boundary condition gives f(0) =f’(O) = 0.

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).

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 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

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.

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

14 Jul 2014: Phys Rev Lett 110(26):268102. 31. Ishikawa T, Pedley TJ (2008) Coherent structures in monolayers of swimming particles.Phys Rev Lett 100(8):088103.

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