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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.

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. &