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  2. Preprint submitted toSAMPLING THEORY IN SIGNAL AND IMAGE PROCESSING…

    www.damtp.cam.ac.uk/research/afha/anders/STSIP_final.pdf
    13 Oct 2017: Foucart and H. Rauhut. A Mathematical Introduction to Compressive Sensing. SpringerScienceBusiness Media, New York, 2013. ... Adam Hilger, Bristol and New York, 1990. [48] C. Shannon. A mathematical theory of communication.
  3. Uniform and high-order practical implementation ofSturm–Liouville…

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2015_04.pdf
    15 Feb 2017: 1 IntroductionThis paper is about the practical implementation of a new algorithm to approximate the eigenvalues andeigenfunctions {(λj,yλj)}jZ0 of regular Sturm–Liouville problems in Liouville’s normal form. ... At the heart of this advancement,
  4. PHYSICAL REVIEW E 93, 023116 (2016) Flow-induced compaction of ...

    www.damtp.cam.ac.uk/user/jneufeld/pubfiles/Hewitt-2016.pdf
    20 Jan 2017: of a new theoretical model. Our experimental setup consistsof a saturated, deformable porous medium that is open to theatmosphere at its base. ... 2(d)] is nota simple reversal of the behavior above. Instead, the porosityat the base instantly adopts a
  5. Magnus expansions and pseudospectra of Master Equations

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2017_01.pdf
    11 Jan 2017: Department of Applied Mathematics and Mathematical Physics, University of Cambridge,Wilberforce Road, Cambridge CB3 0WA, UK (a.iserles@damtp.cam.ac.uk)†School of Mathematics and Statistics, University of New South ... 4. Discussion. Master equations
  6. PHYSICAL REVIEW FLUIDS 2, 093101 (2017) Two-fluid model for ...

    www.damtp.cam.ac.uk/user/lauga/papers/140.pdf
    7 Nov 2017: A. Squirming in a rigidly bounded flow. In the laboratory frame of reference, the boundary conditions at the swimmer surface and theinterface are given for this new model by. ... B. Rewriting theseequations formally as. v̄r (a,θ0) =. n=0Ān(t )Pn(ξ ),
  7. ON THE STABLE SAMPLING RATE FOR BINARY MEASUREMENTS AND ...

    www.damtp.cam.ac.uk/research/afha/anders/Paper.pdf
    13 Oct 2017: To form an orthonormalbasis, we simply apply a Gram-Schmidt procedure. The new functions, after the orthonormalisation, aredenoted by φleftn ,φ. ... Hansen, C. Poon, and B. Roman. Breaking the coherence barrier: A new theory for compressed sensing.
  8. Commutator-free Magnus–Lanczos methods for the linear Schrödinger…

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2017_05.pdf
    3 Oct 2017: 2. 〈f〉0 = f; and. 3. 〈1〉2 = 2x. With this new notation in place and using (2.6), we can now simplify commutatorsto anti-commutators,. ... B̃j(h,ζ) = hjBj (ζ/h). 2.7 Fourth order commutator-free Magnus expansions. With this new notation in place
  9. Fluctuating pseudoatoms in metallic fluids Raymond E. Goldstein…

    www.damtp.cam.ac.uk/user/gold/pdfs/fluctuating_pseudoatoms.pdf
    19 Dec 2017: New York 14853-2501. (Received 6 February 1989; accepted 20 April 1989).
  10. on November 22, 2017http://rsif.royalsocietypublishing.org/Downloaded …

    www.damtp.cam.ac.uk/user/gold/pdfs/filament_oscillations.pdf
    22 Nov 2017: on November 22, 2017http://rsif.royalsocietypublishing.org/Downloaded from. rsif.royalsocietypublishing.org. Research. Cite this article: De Canio G, Lauga E,Goldstein RE. 2017 Spontaneous oscillations of. elastic filaments induced by molecular
  11. Fast expansion on the real line Helge Dietert∗ Arieh ...

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2017_02.pdf
    13 Feb 2017: Firstly, it is possible to manipulate and control particlesby a judicious use of short-burst laser pulses (Kosloff, Rice, Gaspard, Tersigni & Tan-nor 1998, Shapiro & Brumer 2003) and, secondly, a new ... n at thecost of O. (n2). operations – less if

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