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20 Jul 2018: this issue was aired more than 20 years ago by. Adrian Parsegian and Robert Austin (Parse-.

2 Nov 2018: 3.20). On the other hand, if m and n go to infinity in case (6), we consider the expression. ... 20. Figure 3.3: log10 |dm,n| (the blue dotted line) and its asymptotic approximation (thered line), for n = 0 (the top left), m = 0 (the top right), m = n

3 Apr 2018: O(h4)︷ ︸︸ ︷iΛ [ψ]1,1(h) 2i. 〈2xµ2,1(h). 〉2, (2.20). whereψ(h,ζ,ξ) = ζ ξ h3. ... Magnus–Lanczos. In Figure 4.3 (right) and Figure 4.4 (right) we show the errorsin exponentiating the order six Magnus expansions (with and without

19 Jan 2018: Error is satisfying u = 0 (N = 20) as function of t. ... u. x. N=302014. s-w, 28. Re = 10 and N = 14, 20 and 30.Also result from ψ ω formulation at N = 28.

24 Jul 2018: Compressive Imaging (CI), U = ΨHadΦdwt 256256 @ 12.5%. MRI, U = ΨdftΦdwt 10241024 @ 20%. ... S1: Best for 256x256. S2: Best for 2048x2048. 6.73%7.30%. 21.3%20.5%. Recovery error.

13 Apr 2018: As a sanity check forcotton, μ 0.3–0.4 [4,5], and thus, hΘi 20. ... 20] M. Abramowitz and I. A. Stegun, Handbook of MathematicalFunctions (Dover, New York, 1965).

31 Dec 2018: G = F pV = E pV TS (4.20). This is a Legendre transform of F , this time swapping volume for pressure: G = G(T, p). ... already seen in Section 1.4.1. From its definition (4.20), we see that the Gibbs free. –

14 May 2018: 2Fµ dx. µ dx(7.20). where Fµ are the curvature components. Recall that AU is a matrix–valued 1-form, so.

13 Dec 2018: For example, without further approximation,evaluation for a scatterer of around 220 by 20 wavelengthscan be carried out in around 100 minutes using 32processors on the SunFire machine. ... 0.05 0.05 0.2 0.6 1.0 1.4 1.8. Fig. 1 Surface current amplitudes

8 Aug 2018: Received 1 September 1995; accepted 20 December 1995! Molecules at the air–water interface often form inhomogeneous layers in which domains ofdifferent densities are separated by sharp interfaces. ... Hr! 5p. 2r2lnr! 20! and. Gij r! 5 2 d i j lnr!