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4 Aug 2015: B. Liverpool and A. Ajdari, New J. Phys.,2007, 9, 126. 25 J. ... A. Orszag, Advanced Mathematical Methods. for Scientists and Engineers, McGraw-Hill, New York, 1978.39 L.

24 Mar 2015: 3] C. Isenberg, The Science of Soap Films and Soap Bubbles(Dover, New York, 1992).

30 May 2015: Applied and Numerical HarmonicAnalysis. Birkhäuser/Springer, New York, 2013. [Online]. Available:http://dx.doi.org/10.1007/978-0-8176-4948-7. [7] R. ... Adcock, A. C. Hansen, C. Poon, and B. Roman, “Breaking thecoherence barrier: A new theory for

4 Aug 2015: Garland Science, New York, 2014). [2] J. Kärger, T. Binder, C.

30 May 2015: Conf., Belfer Grad. School Sci., Yeshiva Univ., New York,1962–1964), 1966, pp.

5 Aug 2015: Normalizing this new density func-tion, thus making the integral for the total number of bacterialcells appear at the denominator, we finally re-express Eq. ... Springer-Verlag, New York,2003). [21] M. Tindall, P. Maini, S. Porter, and J.

28 May 2015: Other aspects of this new"development have been reported elsewhere (Jaynes 1986, 1988, 1989). ... 2. The Problem. We repeat the familiar story, already told hundreds of times; but with a new ending.

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

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,.

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.

10 Jul 2015: Aiming to spur new research in this direction, we conclude this note with a listof open problems and topics for future research. ... Poon, and B. Roman. Breaking the coherence barrier: A new theory for compressed sensing.arXiv:1302.0561, 2014.

30 Nov 2015: as our new form of Green’s second identity involving Gn, where now we take the boundary.

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].

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].

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.

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

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.

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

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

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,.