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26 Feb 2016: Information Processing Systemsvol 4 (San Mateo, CA: Morgan Kaufmann) pp 1017–24.

12 Jul 2016: Nature443(7110), 409–414 September (2006). [24] Laussy, F. P., Shelykh, I. A., Malpuech, G., and Kavokin,A.

3 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

25 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.

18 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

17 Aug 2016: I. Fourier. transforms’, IMA J. Numer. Anal. 24(3), 365–391. Iserles, A. &

24 Nov 2016: Accepted: 17 October 2016. Published: 24 November 2016. Reviewing editor: Richard M.

8 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

23 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

4 Mar 2016: ux0 þ rðtÞ; t uðx0; tÞþ rðtÞu xðx0; tÞ: (24). As the velocity field, the distance x and the displacement rare made dimensionless using n0x, k.