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Torborg2004
www.damtp.cam.ac.uk/user/sje30/waverepo/fourplot/Torborg2004/zzz/Torborg2004_2002-09-24-1.html28 Jan 2016: -
Stephen J Eglen
www.damtp.cam.ac.uk/user/sje30/pubs.html13 Mar 2016: Frontiers in Computational Neuroscience 7:24. -
Torborg2004
www.damtp.cam.ac.uk/user/sje30/waverepo/fourplot/Torborg2004/zzz/Torborg2004_2002-08-24-1.html28 Jan 2016: -
Stafford2009
www.damtp.cam.ac.uk/user/sje30/waverepo/fourplot/Stafford2009/zzz/Stafford2009_Beta2KO_37C_Ventral_2008-10-24-0.html28 Jan 2016: -
www.damtp.cam.ac.uk/user/mem/oldftp/lucidity-supplem.txt
www.damtp.cam.ac.uk/user/mem/oldftp/lucidity-supplem.txt24 Oct 2016: Stuckness. the predecessor of all real understanding.'' [Near end of chapter 24, p.286 in the original edition.] Of course one can be getting on with other things, at least part -
Torborg2004
www.damtp.cam.ac.uk/user/sje30/waverepo/fourplot/Torborg2004/zzz/Torborg2004_2002-09-24-0.html28 Jan 2016: -
Ferromagnetic and antiferromagnetic order in bacterial vortex lattices
www.damtp.cam.ac.uk/user/gold/pdfs/nphys3607.pdf1 Apr 2016: 8, 899–911 (2013).24. Novoselov, K. S. et al. Two-dimensional gas of massless Dirac fermions in. -
PHYSICAL REVIEW FLUIDS 1, 073201 (2016) Elastohydrodynamic…
www.damtp.cam.ac.uk/user/gold/pdfs/elasto_synchro.pdf1 Nov 2016: large. However, it is well knownthat use of the leading-order approximation of slender body hydrodynamics for larger values of isrobust [24,25]. ... A(τ ) =(. Be2(2k2k4 )τ 3k. 4. 4(2 k2))1/2. (24). 073201-8. -
Cop yrig ht © 201 6 U nive rsity ...
www.damtp.cam.ac.uk/user/examples/A5g.pdf10 Jun 2016: mis. sion. 4 Surfaces and Surface Integrals 24. 4.1 Surfaces and Normals 24. ... 24 –. Cop. yrig. ht. 201. 6 U. nive. rsity. -
Slender-ribbon theory
www.damtp.cam.ac.uk/user/lauga/papers/115.pdf25 Feb 2016: Shortly thereafter, Lighthill proposed a derivation which was accurate toorder 1/2.21,24 This was a vast improvement on the earlier methods but still did not account for theends of ... 2n̂. s. 1. O(b3), (24). R. 0. =b 1,bt̂ b2 21,b. -
Power and limitations of convex formulationsvia linear and…
www.damtp.cam.ac.uk/user/hf323/Fawzi_PhDthesis.pdf6 Oct 2016: 24. 2.2.4 Proof of the factorization theorem for SDP lifts. We now give a proof of Theorem 3. -
Non-resonant optical control of a spinor polariton condensate A. ...
www.damtp.cam.ac.uk/user/ngb23/publications/PRB2016.pdf12 Jul 2016: Nature443(7110), 409–414 September (2006). [24] Laussy, F. P., Shelykh, I. A., Malpuech, G., and Kavokin,A. -
Coordinated beating of algal flagella is mediated by basal coupling
www.damtp.cam.ac.uk/user/gold/pdfs/coupling_pnas.pdf18 May 2016: The basic configurationof two flagella appears in multiple lineages by convergent evolu-tion, e.g., in the naked green alga Spermatozopsis (23), in gametesof the seaweed Ulva (24), and in swarm -
14799850532483 1..16
www.damtp.cam.ac.uk/user/gold/pdfs/aerotaxis_elife.pdf24 Nov 2016: Accepted: 17 October 2016. Published: 24 November 2016. Reviewing editor: Richard M. -
NE7405
www.damtp.cam.ac.uk/user/sje30/papers/network97.pdf26 Feb 2016: Information Processing Systemsvol 4 (San Mateo, CA: Morgan Kaufmann) pp 1017–24. -
mssmRge.eps
www.damtp.cam.ac.uk/user/examples/3P7.pdf8 Mar 2016: Cop. yrig. ht. 201. 6 U. nive. rsity. of C. ambr. idge. Not. to b. e qu. oted. or. repr. oduc. ed w. ithou. t per. mis. sion. Prepared for submission to JHEP. Supersymmetry. B. C. Allanacha F. Quevedoa. aDepartment of Applied Mathematics and -
Noname manuscript No.(will be inserted by the editor) Symmetric ...
www.damtp.cam.ac.uk/user/na/NA_papers/NA2016_01.pdf23 Jul 2016: 24). Finally, inserting (24) into (22) and (23) yields. ‖u(tn1) un1‖ t2r4‖f(2r2)t. ... 24 C. Liu, A. Iserles, X. Wu. For the time integrators Brik1 and Brik2 derived in this paper we use thetolerance 1015 and choose m = 2 in the waveform relaxation -
VOLUME 79, NUMBER 22 P H Y S I ...
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/Fygenson_etal.pdf3 Oct 2016: This is of the same orderas forces generated by specialized motor proteinss,5 pNd[24], and agrees with the scale of force expected from thfree energy calculation (Table I). ... 24] J. T. Finer, R. M. Simmons, and J. A. Spudich, Nature(London) 368, 113 -
J. Fluid Mech. (2015), vol. 777, pp. 97–121. c© ...
www.damtp.cam.ac.uk/user/jneufeld/pubfiles/Pegler-2015.pdf11 Jan 2016: leakage rate predicted by (2.24) is then unphysical because there is no fluidabove the outlet to draw. ... Generally, this assumptionis invalid if the current delivers a smaller flux towards the outlet than is predicted toleak according to (2.24). -
Priscilla Canizares-Martinez Current position: University of…
www.damtp.cam.ac.uk/research/afha/people/priscilla/PCanizares.pdf27 Jan 2016: 09/01/2013 BBC Stargazing LIVE, 2013 (UK): Science exhibit: ”Growing Galaxies. 24/03/2012 Institute of Astronomy Open Day, support staff (UK): Activity Title: “Making a spec-trometer.
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