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22 Nov 2017: Ð L0 k. 2(s, t)ds, with a vanishing intrinsic curvature[24], thus neglecting shearing stresses.

13 Oct 2017: ON THE STABLE SAMPLING RATE FOR BINARY MEASUREMENTS AND WAVELETRECONSTRUCTION. A. C. HANSEN AND L. TERHAAR. ABSTRACT. This paper is concerned with the problem of reconstructing an infinite-dimensional signal from alimited amount of linear

13 Oct 2017: In the last example we used the code from [24] and consider reconstructionof images from Fourier samples. ... J. Amer. Math. Soc., 24(1):81–124, 2011. [30] A. C. Hansen and L.

16 Oct 2017: homozygotes and the microtubules continue to grow at 0.24 mm/sec (Figure 7A).

3 Oct 2017: ζ0. ψ(h,ζ,ξ) dξ dζ = 0, (2.24). lending an extra power of h to terms featuring Λ [ψ]a,b(h).

15 Feb 2017: A , [B, [A , C ]]] = 0, [B, [A , [B, G ]]] = 0, [C , [A , [C , E ]]] = 0, (3.24)[A , [B, [A , E ]]] = 0, [B, [B, [B, C ]]] = 0, [C , [A , [C , G ]]] =

9 Jul 2017: Thus we have a time quasicrys-tal, in analog of a conventional spatial quasicrystal [24].The persistent rotation of trapped ions can be detected. ... 24] D. Levine and P. J. Steinhardt, Phys. Rev. B 34, 596(1986).

13 Oct 2017: ON THE STABLE SAMPLING RATE FOR BINARY MEASUREMENTS AND WAVELETRECONSTRUCTION. A. C. HANSEN AND L. TERHAAR. ABSTRACT. This paper is concerned with the problem of reconstructing an infinite-dimensional signal from alimited amount of linear

19 Dec 2017: y(J) (r I,t l,r2,t2,r3,t3). == ( - i) (T{n(rl,tl)n (r2,t2)n(r3,t3)}), (2.24 ) as the time-order expectation of the electron ... This in tum gives. 24. k = 81T,Be2A i 3XI-'(0), (5.8).

4 Sep 2017: β. IL. βI. Lβ. IL. βI. Lβ. IL. β. β = 0.44ν = 1.24. ... 24] We note that this phase is related to the π spin glass phase[10,13] and is referred to as a Floquet time crystal in [11].