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13 May 2009: Van,cn(α, β, nz) =. 0(t α)a(t β)cenφ(t) dt, (4.23). withφ(t) = zt log(t α) log(t β) (4.24). ... Iserles (DAMTP, University of Cambridge). 24. References. [1] Milton Abramowitz and Irene A.

30 Nov 2009: 24 H. Brunner, A. Iserles & S.P. Nørsett. Figure 3.3: The number of significant digits in approximating one of the two nonzero eigen-values forKω(x, y) = cos ω(x

12 Aug 2009: 12α2 (1 α)2 ‖y. j xk‖4, αR, (4.24). the last line being due to the positive semi-definiteness of =ZZT.

1 Dec 2009: 3.24). The corresponding result is the following. Theorem 2 Let f(y) be constant, then we have θ0 = 0, θ1 = ̺ and. ... θs = (s 1)̺, s 2.Proof We shall use formula (3.24) and proceed along the lines of theproof of Theorem.

13 Jun 2009: The the extension to bivariate functions was developed, without analysis,in [24, 25, 27]. ... The bivariate version of this method wasoriginally developed, without analysis, in [24, 25, 27].

3 Sep 2009: Despite the numerous results already obtained in thefield, therearestillmanyopenproblemsandtherehasbeenaburstof new experimental results in the last few years [24,25,29,31]. ... and also between solitons [24,25,39] still clearly have a lot

3 Sep 2009: R1. 2r0R2. 2. R12. r0 R1 , 24. where a sign has been added to indicate the circulationof the vortex.

18 Jul 2009: 578–594. 24.

6 May 2009: 1–24 of the Collected Papers, Vol. 3, M. Y. Hussaini, Ed., Oxford.

30 Nov 2009: The. 24. cubature points are indicated by dots. Derivatives of increasing order are indicated by cir-cles with increasing radius.