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41 - 50 of 71 search results for TALK:ZA31 24 / |u:www.damtp.cam.ac.uk where 0 match all words and 71 match some words.

  1. Results that match 1 of 2 words

  2. 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

  3. 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].

  4. Stafford2009

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

  5. 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

  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. 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

  8. 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

  9. 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.

  10. Sensing in the Mouth: A Model for Filiform Papillae as Strain…

    www.damtp.cam.ac.uk/user/lauga/papers/124.pdf
    1 Oct 2016: Other measurements reports significantly larger sizes, withwidths that can range 100–300 µm and length 200–500 µm[21, 23, 24]. ... hydrodynamics and flow sensing. Annu Rev Fluid Mech. (2016) 48:1–24. doi:.

  11. jasD140370 1119..1141

    www.damtp.cam.ac.uk/user/mem/thomson-mci-jupiters-unearthly-jets-jas16.pdf
    18 Feb 2016: Manuscript received 9 December 2014, in final form 24 September 2015).

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