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1 May 2024: 2012). 109,. 268102. (doi:Modelling lateral manoeuvres in fish. K Singh, TJ Pedley. – ... 2010). 82,. 021408. (doi:Instability of uniform micro-organism suspensions revisited. TJ Pedley. –

1 May 2024: P Glendinning, JR Gog, WS Hart, H Heesterbeek, T House, M Keeling, IZ Kiss, ME Kretzschmar, AL Lloyd, ES McBryde, JM McCaw, TJ McKinley, JC Miller, M Morris, PD O'Neill,

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

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

1 May 2024: Enterria, M Diefenthaler, M Fucilla, MV Garzelli, M Guzzi, M Hentschinski, TJ Hobbs, J Huston, J Isaacson, SR Klein, F Kling, P Kotko, YV Kovchegov, G Krintiras, AS Kronfeld, K Kutak,

1 May 2024: 1171. (doi: 10.1051/jp2:1993189). Statics and dynamics of self-assembled dipolar rods. TJ DRYE, ME CATES. – ... TJ DRYE, ME CATES. – The Journal of Chemical Physics. (1992).

1 May 2024: Partridge, G Patanchon, TJ Pearson, M Peel, HV Peiris, F Perrotta, V Pettorino, F Piacentini, L Polastri, G Polenta, J-L Puget, JP Rachen, M Reinecke, M Remazeilles, A Renzi, G

1 May 2024: Enterria, M Diefenthaler, M Fucilla, MV Garzelli, M Guzzi, M Hentschinski, TJ Hobbs et al.

1 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

1 May 2024: 349,. 131. (doi: 10.1016/0370-2693(95)00214-6). Integrable theories that are asymptotically CFT. JM EVANS, TJ HOLLOWOOD. – ... JM EVANS, TJ HOLLOWOOD. – Physics Letters B. (1995). 343,. 198.

1 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

1 May 2024: 2002). 66,. 105013. (doi: 10.1103/physrevd.66.105013). Exact superpotentials from matrix models. N Dorey, TJ Hollowood, SP Kumar, A Sinkovics. – ... no. 040. N Dorey, TJ Hollowood, SP Kumar, A Sinkovics. – Journal of High Energy Physics.

1 May 2024: Partridge, G Patanchon, TJ Pearson, M Peel, HV Peiris, F Perrotta, V Pettorino, F Piacentini, L Polastri, G Polenta, J-L Puget, JP Rachen, M Reinecke, M Remazeilles, A Renzi, G

1 May 2024: TJ Howat, C Barreca, P O'Hare, JR Gog, BT Grenfell. – Journal of the Royal Society, Interface.

1 May 2024: Moneti, L Montier, D Mortlock, A Murphy, F Nati, CB Netterfield, HU Norgaard-Nielsen, C North, F Noviello, D Novikov, S Osborne, F Pajot, G Patanchon, T Peacocke, TJ Pearson, O ... B Partridge, F Pasian, G Patanchon, TJ Pearson, O Perdereau, L Perotto, F

1 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

1 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

1 May 2024: J-L Yan, C Li, NR Boonzaier, DM Fountain, TJ Larkin, T Matys, A van der Hoorn, SJ Price. –

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

1 May 2024: Murphy, F Nati, CB Netterfield, HU Norgaard-Nielsen, C North, F Noviello, D Novikov, S Osborne, C Paine, F Pajot, G Patanchon, T Peacocke, TJ Pearson, O Perdereau, L Perotto, F ... B Partridge, F Pasian, G Patanchon, V Pavlidou, TJ Pearson, O Perdereau,

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

1 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,

1 May 2024: DR Brumley, M Polin, TJ Pedley, RE Goldstein. – Physical review letters.

1 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. –

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

1 May 2024: TJ Wang, RJ Thomas, JW Brosius, PR Young, DM Rabin, JM Davila, G Del Zanna. –

1 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. –

1 May 2024: N Dorey, TJ Hollowood. – Journal of High Energy Physics. (2005).

1 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

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

1 May 2024: BP Marinković, A Markwick, T Marquart, HE Mason, NJ Mason, C Mendoza, AA Mihajlov, TJ Millar, N Moreau, G Mulas, Y Pakhomov, P Palmeri, S Pancheshnyi, VI Perevalov, N Piskunov, J

1 May 2024: Enterria, M Diefenthaler, M Fucilla, MV Garzelli, M Guzzi, M Hentschinski, TJ Hobbs et al.

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 =

10 Apr 2011: Magar V, Goto T, Pedley TJ (2003) Q J Mech Appl Math 56:65–91.35.

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.

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.

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:

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

1 May 2024: B Partridge, F Pasian, G Patanchon, V Pavlidou, TJ Pearson, O Perdereau, L Perotto, M Perri, F Perrotta, F Piacentini, M Piat, S Plaszczynski, P Platania, E Pointecouteau, G Polenta, N ... Patanchon, D Pearson, TJ Pearson, O Perdereau, L Perotto, F

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.