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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

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].

28 Jan 2016:

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

28 Jan 2016:

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

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

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.

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:.

18 Feb 2016: Manuscript received 9 December 2014, in final form 24 September 2015).

25 Feb 2016: FL48CH05-Lauga ARI 24 November 2015 12:50. Flagellum: organellecomprising the rotarymotor, hook, andfilament. ... sona. l use. onl. y. FL48CH05-Lauga ARI 24 November 2015 12:50.

12 Aug 2016: for m0 = 3 at (M, N, L) = (8, 24, 5) and α = 2.44. ... 18. Figure 6. The continuation curve for m0 = 3, α = 2.44 at Re = 2200 (Acrit = 1.182 104,truncation (8,24,5)).

22 Jan 2016: algae ingravitational fields [22] and can be treated analytically [23].However, the present internal torques can be treatedanalytically only in two dimensions [24] and numerical[25] or approximative [26] methods are ... 24] S. van Teeffelen and H. Löwen,

6 Oct 2016: i. |hi|2. where := cos(π/N) x F(N,C). 15 / 24. ... and the sos hierarchy needs only dN/4e levels. 24 / 24.

13 Dec 2016: Many surrogate models for flagellar dynamics have been proposed [13–24],typically with a set geometry that fixes the range and coupling between oscillators. ... R. Soc. Interface 10, 20130571 (2013). [24] I. Kavre, A. Vilfan, and D.

28 Jan 2016:

1 Oct 2016: In order to solve Eqs. (1) in the fluid surrounding the nematode, we employ the regularizedstokeslet boundary element method [23,24]. ... Analysis, validation, and application to helical swimming, Phys. Fluids 17, 031504 (2005).[24] D.

2 Nov 2016: large. However, it is well knownthat use of the leading-order approximation of slender body hydrodynamics for larger values of isrobust [24,25]. ... A(τ ) =(. Be2(2k2k4 )τ 3k. 4. 4(2 k2))1/2. (24). 073201-8.

1 Jul 2016: Equation (6) givesthe spatial part of the Lagrangian for a scalar ϕ4 theory onthe circle [24,25], and ϕ may be thought of as analogousto the field u in the SSH ... Acad. Sci. U.S.A. 111, 13004 (2014). [24] N. S. Manton and P.

12 Aug 2016: Formally, the appropriate hydromagnetic inner product (i.e. the modified version of (2.24) taking account of the dipolar field) is required here to suitably weight the momentum and induction equations. ... 2 2 ). ( 3. 2 3 ). (3.24). so that the normal