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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. &