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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

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),