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  2. Why geometric numerical integration? A. Iserles & G.R.W. Quispel…

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2015_05.pdf
    17 Dec 2015: Since its emergence, GNI has become the new paradigm in numerical solution ofODEs, while making significant inroads into numerical PDEs. ... As often, yesterday’srevolutionaries became the new establishment. This is an excellent moment to pauseand take

  3. PHYSICAL REVIEW E 92, 023004 (2015) Phase-separation models for ...

    www.damtp.cam.ac.uk/user/lauga/papers/109.pdf
    4 Aug 2015: Fluid. Mech. 9, 339 (1977).[5] D. Bray, Cell Movements (Garland Publishing, New York, NY,. ... 2009).[7] H. C. Berg, E. coli in Motion (Springer-Verlag, New York, NY,.

  4. Banded, stable, skew-symmetricdifferentiation matrices of high order…

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2015_03.pdf
    9 Nov 2015: McLachlan, and N. Robidoux. Skew-adjoint finite differencemethods on nonuniform grids. New Zealand J. ... Academic Press,New York-London, 1974. mclachlan03sdo [6] R. I. McLachlan. Spatial discretization of partial differential equations withintegrals.

  5. 10 Green’s functions for PDEs In this final chapter ...

    www.damtp.cam.ac.uk/user/dbs26/1BMethods/GreensPDE.pdf
    30 Nov 2015: as our new form of Green’s second identity involving Gn, where now we take the boundary.

  6. Continuous Compressed Sensing of Inelastic and Quasielastic Helium…

    www.damtp.cam.ac.uk/research/afha/anders/CS4HAS_Arxiv_2.pdf
    4 Oct 2015: the characteristics of the approxima-tion in the new basis rather than the truncated Fourier series. ... This new vibrational modes are called surface phononsdue to their localisation at the surface [24–26].

  7. On the absence of the RIP in real-world applications ...

    www.damtp.cam.ac.uk/research/afha/people/alexb/papers/ripl.pdf
    10 Jul 2015: To solve this problem, the new conceptsof asymptotic sparsity, asymptotic incoherence and multi-level sampling were introduced. ... We now introducethe fourth new concept in the new theory of compressive sensing: the RIP in levels.

  8. Numerical stability in the presence of variable coefficients Ernst ...

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2013_10.pdf
    3 Apr 2015: Needless to say, it is but an initial foray into a large and important areaand our results, while solving some long-standing problems, pose many new questions.These questions and further

  9. Scientific Programming with R Stephen EglenLaurent Gatto September 6, …

    www.damtp.cam.ac.uk/user/sje30/teaching/r/2015/spr-4up.pdf
    1 Oct 2015: 1) , or directly by assigning new element (e.g. 2):. > l1 <- list(who="fred"). > ... z ## same as return(x). }. 140 / 191. Example of writing a new function.

  10. J. Fluid Mech. (2014), vol. 757, pp. 330–353. c© ...

    www.damtp.cam.ac.uk/user/jneufeld/pubfiles/Pegler-2014-1.pdf
    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

  11. J. Fluid Mech. (2014), vol. 745, pp. 592–620. c© ...

    www.damtp.cam.ac.uk/user/jneufeld/pubfiles/Pegler-2014.pdf
    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

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