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19 Nov 2014: data[dest 3] = color >>> 24; 1422 src = (j & 1); 1423 dest = 4; 1424 } 1425 src = (i & 1)? ... 3] = color >>> 24; 1454 } 1455 break; 1456 } 1457 }; 1458 1459 / 1460 Render a new frame.

14 Jun 2014: graphical-friendly.I Emacs 23 very stable.I Emacs 24 due out next year? ... Emacs 24 as stable base for documents. 3. Tom Dye has a nice reproducible solution for Org config.

14 Jun 2014: This matches results from mammalian conephotoreceptors and cholinergic amacrine cells [11, 24]. ... retinal studiesVis. Neurosci.6 95–111[24] Rodieck R W and Marshak D W 1992 Spatial density and distribution of choline acetyltransferase.

22 Dec 2014: λq(ck )(tck), (24). where the derivatives η( j)λ ,1(ck,t) R and S( j)λ ,1(ck,t) sl(2,C) can be bounded inde-. ... 24 Alberto Gil C. P. Ramos, Arieh Iserles. References. Driscoll, T., Hale, N.

28 Nov 2014: xx0‖t0t1. e(t1, x) dx. ‖xx0‖t0. e(0, x) dx. (6.24). This implies that if the initial data are zero then the solution is zero at all later ... et p = u2t 0. which gives the same conclusion 6.24 for positive times.

4 Nov 2014: ahX=0-07 exp (V/20), (23)and II V301). Ph --Jrx 10 I(24). 516. ... h=1/(exp V30 1). (24). Equation (26) is derived simply from eqns.

26 Mar 2014: m Cka log(1 p1)log(n),. for some universal constant C > 0 [24]. ... 24]. This raises thequestion of whether there are alternatives which are satisfied by such matrices.

19 Jun 2014: 512. 512. Err 6.01%Err 6.01%. 1024. 10. 24. Err 3.60%Err 3.60%. ... 24), yet it is unclear how areal-world setup can be implemented where signals are sparse in atransform domain.

20 Jul 2014: ranging from! 10 nm to 10 µm.22, 24, 26, 27 Similarly, a liquid interface covered withsurfactants acts as a thin two-dimensional fluid layer separating the liquid phases. ... . ek z. (24). The unknown coefficients in this solution are

23 Jul 2014: Final Example [Feinberg/Zee 1999]. Period 24 Periods 1,. , 24. Simon Chandler-Wilde Spectral Inclusion Sets for Spectra and Pseudospectra. ... Final Example [Feinberg/Zee 1999]. Size 24. Simon Chandler-Wilde Spectral Inclusion Sets for Spectra and

14 Jun 2014: T. Schmidt and M. Buzzard, J. Neurobiol., 1993, 24, 384–399.30 L. ... B. Feller, Neuron, 1999, 24,. 673–685.62 E. Marder and J. M.

14 Jun 2014: 3, 8, 9, 20, and 24). For theother five, however, in situ hybridization revealed a punctatepattern of expression associated with individual muscle fibers(Fig.

4 Nov 2014: P. t= K. 2P. x2(4.24). where the diffusion constant K can be identified as 〈y2〉/2t.THIS SECTION NEEDS MORE WORK!

27 Feb 2014: where. D1 = 2bαα. sinh2(αGt. ). 2αG. , (5.24). D2 = 1α.

14 Jun 2014: Neurosci. 24, 356–369. Jaubert-Miazza, L, Green, E, Lo, F, Bui, K, Mills, J, and Guido, W (2005).“Structural and functional composition of the developingretinogeniculate pathway in the mouse.” Visual ... Neurosci. 14, 1486–1495. Luo, L (2006).

26 Feb 2014: detailed three-dimensional tomographic analysisrevealed that nexins are in fact one and the same with the dyneinregulatory complex, collectively termed the NDRC [24].

29 Aug 2014: parameter, %. We thuswrite. u(0) = u0 % u% O (%2), (24). p(0) = p0 % p% O (%2), (25). ... û% = 0. (31)The fist boundary condition satisfied by the corrective flow û% is found by Taylor expanding theboundary condition (21) to the first order in %.

19 Jun 2014: 512. 512. Err 6.01%Err 6.01%. 1024. 10. 24. Err 3.60%Err 3.60%. ... 24), yet it is unclear how areal-world setup can be implemented where signals are sparse in atransform domain.

31 May 2014: 24. The editorial process Once you’ve submitted a paper to a journal, it followsa set pattern:.

12 May 2014: 24. More simple properties1. A useful result. Let uS (x) be a Stokes flow with F = 0 in V , and let u(x) be anyother incompressible flow, then. ... uixj. =. xj. (σSijui. )σSijxj=F=0. ui (4). Hence result by divergence theorem.24.

6 Oct 2014: ǫABǫF ′Q′C̃A′B′E′Q′ ǫAB(ǫA′E′ǫ. F ′. B′ ǫF ′. A′ ǫB′E′)R. 24+ ǫA′B′ǫ. ... 24. a,b holomorphic functions on C. For these to agree we require.

21 Oct 2014: Image Processing for Fluid Dynamics.  Stuart Dalziel. DL Research Partners 1993 – 2001. Version 2.3  DL Research Partners; September 2001 1. Contents Contents.1. 1 Concept.1. 2 DigImage: Particle Tracking.3 2.1 IMAGE CAPTURE. 3 2.2 PARTICLE

21 Oct 2014: πFn(θ φ) dφ = f(θ) , (1.24). – 8 –. using property ii) of the Fejér kernel.

30 Aug 2014: t(t v). ], (1.24). where t and n are, respectively, the local tangent and normal vectors along the filament. ... 1.24), up to the unknown translational and rotational velocities,(U,), which will be determined by imposing the overall force-free and

28 Nov 2014: Pg ρ0. r<. wb dV (24). and thus we obtain the scaling relation. ... ρ0a4. )a3 = D. 24. μa7, (53). where we have substituted κ/N 2 = 4/ν.

9 Sep 2014: For example, it is nowpossible to measure the force required to hold a swimmingspermatozoon [24–26], alga [27] or bacterium [28] in an opticaltrap.

21 Oct 2014: DiDiDiDiggggImage: DigiFile Utility Index. Version 2.3  DL Research Partners September 2001 24.

13 Jul 2014: Arakawa’s method is used for evaluation of thePoisson bracket.24 The time stepping algorithm is the third.

22 Jan 2014: Received 8 April 2013; revised 24 September 2013; accepted 7 October 2013;first published online 25 November 2013).

24 Jun 2014: wavelet basis,namely using boundary wavelets [24, Section 7.5.3]. ... 1,p], boundary scaling functions andwavelets (using the same notation as in [24] 8).

30 Jul 2014: Funding: See page 14. Received: 11 March 2014Accepted: 24 June 2014Published: 29 July 2014.

14 Jun 2014: 0.24 162 20.0.

6 Oct 2014: components, the possible holonomy groups of these irreducible non–symmetric. Riemannian manifolds have been classified by Berger [24]. ... τ := ξA′(dξA. ′ ξB. ′ΓA. ′B′. ). (2.24). Using τ, we can lift the vector fields ξA′AA′ to F

6 Nov 2014: In three dimensions the general solution of (2.24)-(2.25) depends on four arbi-. ... 3.16). 24. Note that R acts on δf without ambiguity (alternatively, the ambiguity in bound-.

14 Jun 2014: 14 Stephen J. Eglen. mean (µm). s.d. (µ. m). 15 16 17 18 19 20 21 22 23 24 25.

14 Jun 2014: gr o u n d ( x )r o u n d ( x , d i g i t s = 2 ). Let’s see how this works in more detail. 24 / 1.

14 Jun 2014: Received Dec. 27, 2002; revised June 24, 2003; accepted July 2, 2003.This work was funded by the Biotechnology and Biological Sciences Research Council (E.S.) and the Wellcome.

8 Dec 2014: A =. kT log 2 1β. log[1 β2(qJM h)2/2 β4(qJM h)4/24. ]. ... hA1/24. |A2|3/2. A4 is not particularly interesting: the denominator |A2| is the interesting part.

14 Jun 2014: Axons first innervate/reachtargets. 5P0 E32 E16 E6 E16 E35 E21[23] [24] [25] [2] [26] [27]. ... 1981); 24: Shatz (1983); 25: Bunt et al. (1983); 26: Godement et al.(1984); 27: Crabtree (1990); 28: Wong et al.

21 Feb 2014: wavelet basis,namely using boundary wavelets [24, Section 7.5.3]. ... 1,p], boundary scaling functions andwavelets (using the same notation as in [24] 8).

14 Jun 2014: gr o u n d ( x )r o u n d ( x , d i g i t s = 2 ). Let’s see how this works in more detail. 24 / 1.

12 Jan 2014: the higher resolution obtained and the lower magnetic gradientsrequired to scan along such trajectories [24, 28, 31]. ... Note that our analog modelis the same as that used with great success in recent work of Guerquin-Kern, Haberlin, Pruessmann& Unser

28 Nov 2014: 2.5.24)r Note that the convolution theorem derived here. uNow return to the key condition in Eq. ... 8ÿ. n“0. 1. n! ˆ. it. ˙n. Hn. (4.2.3). 4 PICTURES AND OPERATORS 24.

10 Jun 2014: Analyzing the Structure of Multidimensional CompressedSensing Problems through Coherence. A. JonesUniversity of Cambridge. B. AdcockPurdue Univesity. A. HansenUniversity of Cambridge. Abstract. In previous work it was established that asymptotic

23 Mar 2014: 23. 4.3 The Peano kernel theorem. 23. 4.3.1 Examples. 24. 4.3.2 Where does K(θ) vanish?

31 May 2014: Weighted Fourier frames, which we also refer to as weighted frames of exponentials, werestudied by Gröchenig [25], and later also by Gabardo [24].

8 Mar 2014: Linear Stable Sampling Rate: Optimality of 2D WaveletReconstructions from Fourier Measurements. Ben Adcock, Anders C. Hansen, Gitta Kutyniok, and Jackie Ma. March 1, 2014. AbstractIn this paper we analyze two-dimensional wavelet reconstructions from

24 Apr 2014: c̃1ρ+ c̃1 φ̃0. ρ=(c c̃0)φ̃1. ρk(ζ)Da k(ζ)c̃0. (3.24). Phoretic self-propulsion at finite Péclet numbers 581.

24 Sep 2014: o. S2. n̂. 24 Typeset by W.I. Jay. Chapter 5. Representations of Lie Groups. ... Definition 24. A representation d of L(G) acting on a vector space V is a linear action v 7 d(X)v,with X L(G) and v V , satisfying.

5 Mar 2014: 610, L137–-L140, doi:10.1086/423305 (2004). 24. Fowler, L. A., Foukal, P. V. &