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41 - 50 of 72 search results for katalk:PC53 24 / |u:www.damtp.cam.ac.uk where 0 match all words and 72 match some words.

  1. Results that match 1 of 2 words

  2. Analyzing the structure of multidimensional compressedsensing…

    www.damtp.cam.ac.uk/research/afha/people/anders/dDCoherence_Arxiv.pdf
    24 Oct 2016: There is a wide variety of problems that lack incoherence, a fact that has been widely recognized [2,6, 10, 11, 24, 25, 27, 33–36, 40], however, they instead posses

  3. Breaking the coherence barrier: A new theory forcompressed sensing ...

    www.damtp.cam.ac.uk/research/afha/anders/BreakingCoherenceRevisionFinal.pdf
    2 Nov 2016: Breaking the coherence barrier: A new theory forcompressed sensing. B. AdcockSimon Fraser Univ. A. C. HansenUniv. of Cambridge. C. PoonUniv. of Cambridge. B. RomanUniv. of Cambridge. Abstract. This paper presents a framework for compressed sensing

  4. Complexity Issues in Computing Spectra, Pseudospectra and Resolvents…

    www.damtp.cam.ac.uk/research/afha/anders/Banach_Hansen_Nevanlinna_edit2.pdf
    22 Oct 2016: For other papers related to the ideas presented in this papers we refer to[3, 4, 6, 10, 11, 12, 13, 14, 15, 16, 17, 24, 26, 30].

  5. Stafford2009

    www.damtp.cam.ac.uk/user/sje30/waverepo/fourplot/Stafford2009/zzz/Stafford2009_Beta2KO_37C_Nasal_2008-10-24-2.html
    28 Jan 2016:

  6. Stafford2009

    www.damtp.cam.ac.uk/user/sje30/waverepo/fourplot/Stafford2009/zzz/Stafford2009_WT_37C_Dorsal_2008-02-08-0.html
    28 Jan 2016:

  7. Breaking the coherence barrier: A new theory forcompressed sensing ...

    www.damtp.cam.ac.uk/research/afha/people/anders/BreakingCoherenceRevisionFinal.pdf
    2 Nov 2016: Breaking the coherence barrier: A new theory forcompressed sensing. B. AdcockSimon Fraser Univ. A. C. HansenUniv. of Cambridge. C. PoonUniv. of Cambridge. B. RomanUniv. of Cambridge. Abstract. This paper presents a framework for compressed sensing

  8. Stresslets Induced by Active Swimmers Eric Lauga1,* and Sébastien ...

    www.damtp.cam.ac.uk/user/lauga/papers/125.pdf
    1 Oct 2016: The stresslet also controlsthe interactions of active organisms with their environment[21,22], enhanced transport through biological fluids[23,24], and the rheology of active fluids [25].If the stresslet of ... cζ dζ: ð26Þ. Using Eq. (24), the

  9. lecture9.dvi

    www.damtp.cam.ac.uk/user/rrk26/Papers/lecture9.pdf
    12 Aug 2016: Re2ν = 0. (24). The last equation is the ‘dual (or adjoint) linearized Navier-Stokes equation’. ... Step.3 Backwards time integrate the dual linearized Navier-Stokes equation (24) with in-compressibility (14) and boundary condition (13) from t = T

  10. lecture7.dvi

    www.damtp.cam.ac.uk/user/rrk26/Papers/lecture7.pdf
    12 Aug 2016: û(x, t) = ũ(y)eikzσt (24). (known to be critical for the energy stability problem), (23) becomes. ... Rev. FluidMech., 43 (2011), pp. 1–24. [12] M. Nagata, Three-dimensional finite-amplitude solutions in plane Couette flow: bi-furcation from

  11. PHYSICAL REVIEW E 93, 043125 (2016) Rotation of slender ...

    www.damtp.cam.ac.uk/user/lauga/papers/119.pdf
    1 Oct 2016: For example, some eukaryoticmicroorganisms have evolved hairs along their flagella calledmastigonemes [23,24]. ... F(t ) = ζ. Udef ds = {0,0,0}, (24). L(t ) = ζ.

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