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16 May 2024: TJ McKinley, PR Murcia, JR Gog, M Varela, JLN Wood. – PLoS Comput.

16 May 2024: RW Ogburn, A Orlando, L Pagano, F Pajot, R Paladini, D Paoletti, B Partridge, F Pasian, G Patanchon, TJ Pearson, O Perdereau, L Perotto, V Pettorino, F Piacentini, M Piat, D

16 May 2024: TJ Pedley, DR Brumley, RE Goldstein. – J Fluid Mech. (2016).

16 May 2024: PA Loboda, HE Mason, C Mendoza, TJ Millar, LA Nunez, VI Perevalov, LS Rothman, E Roueff, TA Ryabchikova, A Ryabtsev, S Sahal-Brechot, VG Tyuterev, V Wakelam, CJ Zeippen. –

16 May 2024: 349,. 131. (doi: 10.1016/0370-2693(95)00214-6). Integrable theories that are asymptotically CFT. JM EVANS, TJ HOLLOWOOD. –

16 May 2024: Montier, G Morgante, A Moss, S Mottet, M Münchmeyer, P Natoli, HU Nørgaard-Nielsen, CA Oxborrow, L Pagano, D Paoletti, B Partridge, G Patanchon, TJ Pearson, M Peel, HV Peiris, F

16 May 2024: JR Gog, A Murcia, N Osterman, O Restif, TJ McKinley, M Sheppard, S Achouri, B Wei, P Mastroeni, JLN Wood, DJ Maskell, P Cicuta, CE Bryant. –

16 May 2024: K Drescher, KC Leptos, I Tuval, T Ishikawa, TJ Pedley, RE Goldstein. –

16 May 2024: PW Mote, TJ Dunkerton, ME McIntyre, EA Ray, PH Haynes, JM Russell. –

16 May 2024: eLife. (2020). 9,. e58635. (doi: 10.7554/elife.58635). Stability of dancingVolvox. T Ishikawa, TJ Pedley, K Drescher, RE Goldstein. –

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

24 Nov 2006: K} such that. ti º tj , j = 1, 2,. , ... K. If ti tj for all j 6= i, we let (ti, ti1,. ,

18 May 2022: operate within the framework of Stokesflow, where the relationship between the dynamics (forcesFj and torques Tj) and kinematics (linear and angularvelocities Uj and Ωj) of rigid bodies is linear.

10 Apr 2011: Nature 2001; 413: 39–44. Wilson DR, Beveridge TJ: Bacterial f lagellar fila-ments and their component f lagellins.

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

16 May 2024: G Patanchon, T Peacocke, TJ Pearson, O Perdereau, L Perotto, F Piacentini, M Piat, S Plaszczynski, E Pointecouteau, R Pons, N Ponthieu, G Prezeau, S Prunet, JL Puget, WT Reach, C ... B Partridge, F Pasian, G Patanchon, TJ Pearson, M Peel, O Perdereau, L

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

3 Jun 2015: on June 3, 2015http://rsif.royalsocietypublishing.org/Downloaded from. rsif.royalsocietypublishing.org. ResearchCite this article: Brumley DR, Polin M, PedleyTJ, Goldstein RE. 2015 Metachronal waves in. the flagellar beating of Volvox and their.

12 Aug 2016: P:?tJ. )3 ,0g 0! 0 aW TU ,! V ,=0 v L:s!

16 May 2024: DR Brumley, M Polin, TJ Pedley, RE Goldstein. – Journal of the Royal Society, Interface.

16 May 2024: AI Malz, R Hlozek, TJ Allam, A Bahmanyar, R Biswas, M Dai, L Galbany, EEO Ishida, SW Jha, DO Jones, R Kessler, M Lochner, AA Mahabal, KS Mandel, JR Martinez-Galarza,

5 Oct 2013: 2. where T = [1, 1) is the unit torus). Given the Fourier coefficients of f , we would like to reconstruct in theorthonormal basis of Chebyshev polynomials φj (x) = cj Tj (x) ... Given that the first kind Chebyshev polynomials Tj are orthogonal with.

1 Sep 2011: More details on the problems relevant to k;p can befound in [1],[2],[5].Recall that Nj(t) := (tjk tj) [tj; tj1; : : :; tjk] ( t)k1+ ;so that suppNj = (tj; tjk); ... degree p such thatsuppMj;p = (tj; tjp1); Z tjp1tj Mj;p(x)dx = 1;and by!

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

1 Apr 2024: Preprint typeset in JHEP style - HYPER VERSION January 2016. The Quantum Hall EffectTIFR Infosys Lectures. David Tong. Department of Applied Mathematics and Theoretical Physics,. Centre for Mathematical Sciences,. Wilberforce Road,. Cambridge, CB3

16 May 2024: UNDERFLIGHT CALIBRATION OF SOHO/CDS AND HINODE/EIS WITH EUNIS-07. TJ Wang, RJ Thomas, JW Brosius, PR Young, DM Rabin, JM Davila, G Del Zanna. –

24 Feb 2005: ωw0,.,wn (tj; tj)> 0. PROOF. We omit to write the weight functions wm here as well. ... Thus,. α. ε=ω(tj; t(ε))ε ω(tj; tj). ε0. ω′(tj; t). ω(tj; tj).

23 Mar 2023: Group Theory Lecture Notes. Hugh Osborn. latest update: March 22, 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

21 Feb 2022: Day et al. eLife 2022;11:e72707. DOI: https:// doi. org/ 10. 7554/ eLife. 72707 1 of 28. Cellular organization in lab- evolved and extant multicellular species obeys a maximum entropy lawThomas C Day1, Stephanie S Höhn2, Seyed A Zamani- Dahaj1,3,4

12 Feb 2018: G(ti, tj ) and further integrals, and so are again suppressed by higher powers of M.

20 Jun 2011: 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