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5 May 2015: ε(2k1)σ1. )for k 2. In these new splittings terms. of size O(ε(2k)σ1. ... With this new notation. in place, the Magnus expansions Θ̃ε3 and Θ̃ε4 can be presented more concisely,.

21 Jan 2015: 2Faculty of Science, University of Bristol, Bristol BS8 1UH, UK3School of Mathematics and Statistics, University of New South Wales, Sydney,. ... We also reveal the new asymptotic regimesthat emerge when the injected fluid is more viscous than the

3 Jun 2015: Because the drag is not isotro-pic, the trajectory of an isolated sphere will deviate slightlyfrom the prescribed circle (dr=r0 0:5% here) to a new limitcycle (r(t),

21 Jan 2015: 2Faculty of Science, University of Bristol, Bristol BS8 1UH, UK3School of Mathematics and Statistics, University of New South Wales, Sydney, NSW 2052, Australia4BP Institute and Department of Earth Sciences, University of ... The former is a new

8 Nov 2015: Θφµ1,.µn(x)Θ1 = (1)nφµ1,.µn(x)†. (1.118). Note that this result is consistent with forming new fields by taking derivatives,e.g.

16 May 2015: One contribution of 10 to a theme issue. ‘Bioinspiration of new technologies’.

27 Apr 2015: The kissing polynomials and their. Hankel determinants. Alfredo Deaño, Daan Huybrechs and Arieh Iserles. April 28, 2015. Abstract. We study a family of polynomials that are orthogonal with respect to theweight function eiωx in [1, 1], where ω 0.

23 Sep 2015: point of the system. Computation of 3D flow fields for each realisation in the new ensemble (3D mean:.

25 Sep 2015: Our understanding of the swimming dynamics of microorganisms has advanced over the past fewdecades in part through the development of new technologies. ... 2003, Pepper et al. 2010). Thissection considers two problems involving the swimming of organisms

18 May 2015: Part II Dynamical Systems Michaelmas Term 2014. lecturer: Professor Peter Haynes (phh1@cam.ac.uk). May 18, 2015. These lecture notes, plus examples sheets and any other extra material will be madeavailable at