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Analyzing the structure of multidimensional compressedsensing…
www.damtp.cam.ac.uk/research/afha/people/anders/dDCoherence_Arxiv.pdf24 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 -
Breaking the coherence barrier: A new theory forcompressed sensing ...
www.damtp.cam.ac.uk/research/afha/anders/BreakingCoherenceRevisionFinal.pdf2 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 -
Complexity Issues in Computing Spectra, Pseudospectra and Resolvents…
www.damtp.cam.ac.uk/research/afha/anders/Banach_Hansen_Nevanlinna_edit2.pdf22 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]. -
Stafford2009
www.damtp.cam.ac.uk/user/sje30/waverepo/fourplot/Stafford2009/zzz/Stafford2009_Beta2KO_37C_Nasal_2008-10-24-2.html28 Jan 2016: -
Breaking the coherence barrier: A new theory forcompressed sensing ...
www.damtp.cam.ac.uk/research/afha/people/anders/BreakingCoherenceRevisionFinal.pdf2 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 -
Stafford2009
www.damtp.cam.ac.uk/user/sje30/waverepo/fourplot/Stafford2009/zzz/Stafford2009_WT_37C_Dorsal_2008-02-08-0.html28 Jan 2016: -
lecture9.dvi
www.damtp.cam.ac.uk/user/rrk26/Papers/lecture9.pdf12 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 -
lecture7.dvi
www.damtp.cam.ac.uk/user/rrk26/Papers/lecture7.pdf12 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 -
PHYSICAL REVIEW E 93, 043125 (2016) Rotation of slender ...
www.damtp.cam.ac.uk/user/lauga/papers/119.pdf1 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. -
Sensing in the Mouth: A Model for Filiform Papillae as Strain…
www.damtp.cam.ac.uk/user/lauga/papers/124.pdf1 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:.
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