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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.

19 Oct 2018: 2.24). Notably, this expression can be simplified into. s0 =sb(rc) r s(.

27 Feb 2018: Resource-explicit models of bacterial mutualismscompare well with experiments in which mutualists are wellmixed [5,6,23,24].

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.

3 Apr 2018: h7), (2.23). Magnus–Lanczos methods with simplified commutators 15. where. ϕ1(h,ζ,ξ) = h2 4hξ 2ζξ, (2.24).

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.

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.

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.

13 Dec 2018: 2.1. Formal solution and splitting series. The method of solution is analogous to that applied to the electromagneticproblem in 2-d or 3-d [23, 24]. ... 24] M. Spivack, J. Ogilvy, C. Sillence, Electromagnetic scattering by large com-plex scatterers in 3d,

16 Jul 2018: Phys. Fluids 24, 061901 (2012). 18. Lauga, E. Bacterial hydrodynamics. Annu. ... 24. Johnson, R. E. An improved slender-body theory for Stokes flow.