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11 May 2017: For finite action solutions to the Euler Lagrange equations (II.24), the fields |B|,|DΦ| and. ... 0. (iii) a(; z) and φ(, z) solve the Euler Lagrange equations (II.24) at λ = 1.

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

6 Jul 2017: While thesubject of sparse quasi-Newton methods was eventually developed mostly by Toint,it also involved Mike in three interesting contributions [24, 26, 31], the first of whichis an extension to

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