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7 Nov 2017: 0.95 3.58–3.68 14.5 μm (1.9–4.3) 103U/U0 0.99 6.24–6.30 25 μm (1.3–2.6) 104U/U0 0.999 ... 0.049U/U0 0.95 3.58–4.04 15.2 μm 0.0020–0.022U/U0 0.99 6.24–6.91 26.3 μm (0.34–4.2)

10 Aug 2017: Clement, and R. Soto, Phys. Fluids 24,. 011901 (2012).[6] S. E. ... 24] H. Wioland, F. G. Woodhouse, J. Dunkel, and R. E.

20 Jan 2017: Received 24 June 2015; revised manuscript received 1 January 2016; published 24 February 2016). ... 24)] while the effective permeability decreases like H1(cf. (22)). The porosity also approaches an asymptotic profilewith φ0 0 as H.

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.

12 Jul 2017: water and the microbeadsuspension were made of glass and polytetrafluoroethylene andfitted with stainless steel needles (24-gauge injection needles;Carl Roth GmbH), and the inlet and outlet reservoirs were madeof glass. ... 4 A, B, and D), at a frame

11 Dec 2017: By this agent the height was depressed to 24, which shows th a t the tension of a surface of soapy water is much less than the combined tensions of a

23 Apr 2017: 23). From (22) and (23)PJL. For a given power P and frequency / , equation (24) gives a maximum value ofuwhen ,X. ... the observed value is 24/14.

10 Nov 2017: These range over geometry in the study of hyper-Kähler manifolds[14,19–23], conformal, Cauchy–Riemann CR and projective structures [24–36], exoticholonomy [37–40], in representation theory [12,41], ... See [41] for details of these constructions,

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.

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

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].