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Can everything be computed? On the Solvability Complexity Index and…
www.damtp.cam.ac.uk/research/afha/workshops/cid2014/Hansen.pdf23 Jul 2014: H ). Then. SCI(Ξ1, )R 2, SCI(Ξ2, 1)R 2. 24 / 26. Tests with the Operator Ψ(Q) for Ψ L(R). -
Digital Object Identifier (DOI) 10.1007/s00220-014-2046-5Commun.…
www.damtp.cam.ac.uk/user/md327/DT14.pdf25 Jul 2014: Received: 24 May 2013 / Accepted: 25 November 2013Published online: 24 April 2014 – Springer-Verlag Berlin Heidelberg 2014. ... ̂α :=(π̂A′α̂A. )=. (πA′. αA ϒA B′π B′). (4.24). Our approach is very much in the spirit of [2]. -
Rhythmicity, Recurrence, and Recovery of Flagellar Beating Kirsty Y.…
www.damtp.cam.ac.uk/user/gold/pdfs/rhythmicity.pdf2 Dec 2014: correlated across multiple scales. In the first instance wecan derive a scalar measure a via a detrended fluctuationanalysis to characterize an individual time series [24], asfollows. ... Lodha, and M. Schroda, Plant J. 52,286 (2007). [24] C.-K. Peng, S. -
Arbitrary–order trigonometric Fouriercollocation methods for…
www.damtp.cam.ac.uk/user/na/NA_papers/NA2014_03.pdf23 Oct 2014: 7, 13, 22–24, 33, 34, 39]. We consider the quadratic in-variant Q = qT Dp of (1). ... u(h) = p0 hk. l=1. blf (vl),. (24). where h is the stepsize, cl, bl, l = 1, 2,. , -
Emacs Lisp List
www.damtp.cam.ac.uk/user/sje30/emacs/ell.html24 Dec 2014: Emacs Lisp List. Last updated: Wed Dec 24 11:36:00 2014. 1270 entries. ... Sat 24 Jun 2006. Update ell.el to point to ELL at Cambridge. -
RAPID COMMUNICATIONS PHYSICAL REVIEW E 89, 060701(R) (2014) Optimal…
www.damtp.cam.ac.uk/user/lauga/papers/91.pdf23 Jun 2014: Theoptimal stroke pattern of Purcell’s finite three-link swimmerwas found by Tam and Hosoi [23], who then went on toconsider optimal gaits for the green alga Chlamydomonas[24]. ... Rev. Lett. 98, 068105 (2007).[24] D. Tam and A. E. Hosoi, Proc. -
DOI 10.1140/epje/i2014-14060-y Regular Article Eur. Phys. J. E (2014) …
www.damtp.cam.ac.uk/user/lauga/papers/94.pdf29 Aug 2014: 24–26]. In this case, thepropulsion, which is impossible to achieve in an isotropicmedium, is enabled by the presence of a wall which breaksthe symmetry of the nearby environment. ... sinh(n 1/2)(α β). [e(n1/2)α sinh(n 1/2)β. e(n1/2)β sinh(n 1/2)α -
Quantum Dynamics of Supergravity David Tong Crete, September 2014 ...
www.damtp.cam.ac.uk/user/tong/talks/crete.pdf4 Sep 2014: µJµ5 =1. 24 16π221N3/2 N1/2. Rµνρσ Rµνρσ (3.5). For us, N1/2 = 0 and N3/2 = 1. ... The. distinction between rigid and gravitational theories was stressed, in particular, in [24]). -
Modeling quantum fluid dynamics atnonzero temperaturesNatalia G.…
www.damtp.cam.ac.uk/user/ngb23/hunt.pdf26 Mar 2014: g., velocity statistics (20–22) andpressure (23)] show starkly different behavior––see, e.g., therecent reviews (24, 25). ... Phys Rev Lett 82(24):4831–4834.9. Kobayashi M, Tsubota M (2005) Kolmogorov spectrum of superfluid turbulence:. -
PHYSICAL REVIEW E 89, 043011 (2014) Geometry and wetting ...
www.damtp.cam.ac.uk/user/lauga/papers/88.pdf22 Apr 2014: This hypothesis isconfirmed by numerical simulations performed using Brakke’sSURFACE EVOLVER [24] and shown in Fig. ... We useSURFACE EVOLVER [24] to analyze the system behavior,illustrating the results with θE = π/2 and 3π/4.
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