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  2. Recovery of a Variable Coefficient in a Coastal Evolution Equation

    www.damtp.cam.ac.uk/user/ms100/PAPERS/JCP99.pdf
    13 Dec 2018: F′n1, An,n =τ. 2ξF′n. (24). This is easily and rapidly inverted by back-substitution.
  3. On asymptotic structure in compressed sensingBogdan Roman ∗, Ben ...

    www.damtp.cam.ac.uk/research/afha/people/anders/Asymptotic_10a.pdf
    24 Jul 2018: 512. 512. Err 6.01%Err 6.01%. 1024. 10. 24. Err 3.60%Err 3.60%. ... This can be coupled with hidden Markov treesto model the wavelet structure, such as in the Bayesian CS (22, 23)and TurboAMP (24) algorithms.
  4. J. Fluid Mech. (2018), vol. 856, pp. 921–957. c© ...

    www.damtp.cam.ac.uk/user/lauga/papers/152.pdf
    19 Oct 2018: 2.24). Notably, this expression can be simplified into. s0 =sb(rc) r s(.
  5. Microbial mutualism at a distance: The role of geometry in diffusive…

    www.damtp.cam.ac.uk/user/gold/pdfs/mutualism.pdf
    27 Feb 2018: Resource-explicit models of bacterial mutualismscompare well with experiments in which mutualists are wellmixed [5,6,23,24].
  6. Collective dissolution of microbubbles

    www.damtp.cam.ac.uk/user/lauga/papers/145.pdf
    18 Apr 2018: Note that this second casepresents many formal similarities with the dissolution process of droplets [22], their evaporation[23], and even dissolving solids [24]. ... 2)P ′n(μ), (24). Un(η) = An cosh(n 12. )η Bn sinh.
  7. Magnus–Lanczos methods with simplified commutators for the…

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2018_01.pdf
    3 Apr 2018: h7), (2.23). Magnus–Lanczos methods with simplified commutators 15. where. ϕ1(h,ζ,ξ) = h2 4hξ 2ζξ, (2.24).
  8. statphys

    www.damtp.cam.ac.uk/user/tong/statphys/three.pdf
    31 Dec 2018: 23. 1. z. 4p2+. (3.24). The next part’s a little fiddly. ... 1. 1. 2p2. 3N. V+. which we then substitute into (3.24) to get.
  9. 1 Foundations of statistical physics 1.1 Density operators In ...

    www.damtp.cam.ac.uk/user/hsr1000/stat_phys_lectures.pdf
    26 Jan 2018: S k log G = kαN log E const. (1.24). and hence.
  10. 16 Aug 2018: X δ. δMSqo =. [ψ̄Xψ. ], X† = X , Jµα =. δ. δAψµαSqo =. [ψ̄γµTαψ. ]. (4.24). As a consequence of invariance under (4.21), for η = η̄ = 0,. ... S̃(1)o =1. 16π2ε. ((nV 2nF ). 1. 180(3F G) 1. 24(2nV nF )RαβγδRαβγδ.
  11. Efficient boundary integral solution for acoustic wave scattering by…

    www.damtp.cam.ac.uk/user/ms100/PAPERS/arxiv1407.5560v1.pdf
    13 Dec 2018: elements. (Bn)mj = Anmnj. (24). We thus require. bn = B1n cn (25). ... from rough surfaces, Waves in Random Media, 6, 151-167 (1996). [24] A.A.

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