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21 Apr 2009: Multivariate modified Fourier series and application to boundary. value problems. Ben AdcockDAMTP, Centre for Mathematical Sciences. University of CambridgeWilberforce Rd, Cambridge CB3 0WA. United Kingdom. March 25, 2009. Abstract. In this paper we

20 Sep 2009: Employment has fallen 24,000 in the last quarter. Unemployment now 6.5 per cent (4.6 per cent a year ago).

20 Sep 2009: you will help save paper. Responses needed by Tue 24 November 2009.

16 Jan 2009: n E|. =1. ǫ0σ (23). nE|. = 0. (24). b). Let S carry current density s per unit length (charge crossing unit length in S in unittime).

29 Jan 2009: 24. Recall Section 1.6: A is not unique, because we can transform the vector potential according to.

16 Oct 2009: An estimate of the hydrodynamic coupling between twoidealized flagella [24] is est ’ rRL. ... E.Goldstein, Science 325, 487 (2009). [24] T. Niedermayer, B. Eckhardt, and P.

31 Jul 2009: www.sciencemag.org SCIENCE VOL 325 24 JULY 2009 489. REPORTS. on. July. ... 24 JULY 2009 VOL 325 SCIENCE www.sciencemag.org490. REPORTS. on. July. 24,.

30 Aug 2009: 2007) 24–26% 40%(Ridgwell and Hargreaves 2007) 34%(Montenegro et al. 2007) 52%. ... Ambio 24(6):376–378Torn MS, Harte J (2006) Missing feedbacks, asymmetric uncertainties, and the underestimation of future.

3 Sep 2009: V|ψ|2 dx = ψ2u v, (24). where v =. V dx, and by ψ the wavefunction of the bulk: ψ ψ as r. ... For thequartic term in the expression for the energy, we write using equation (24).

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

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.