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31 Oct 2002: 24). where. is the weight associated with each grid point. Here a contravariant-to-covariant tensor correction is needed when this gradient is used to calculate the search direction during a ... restricted to its spherical region. For this reason in

29 Oct 2002: Our implementation follows the simplified version of Millam and Scuseria [24].

24 Jan 2002: f̃(ω) =. dt f(t)eiωt ; f(t) =1. 2π. dω f̃(ω)eiωt (24). ... G(x,t) = dωdk. (2π2). ei(kxωt). ρω2 iγω Tk2(29). A. (24 January 2002) (TURN OVER.

12 Sep 2002: 1985), 24-41. [CGW] F. Chung, R. L. Graham and R. M.

2 Feb 2002: 3.1 Hidden mode models for HMM’s 24. v. vi. 3.2 Subband and Multi-Stream based models 26.

24 Sep 2002: 2 (24). Nonlinear Schrödinger equation 5. At best, this describes the phonon branch of the excitation spectrum. ... e.g. see [34]. It is clear from (24) that is negligibly small when , because then!

31 Oct 2002: The equilibrium bond length for this case differs by 3.34% from CASTEP, as compared to -1.24% for the.

9 Sep 2002: Soc. Brasil. Mat. 9 (1978). 83–87.[24] G. P. Scott, ‘A new proof of the annulus and torus theorems’, Amer.

20 Aug 2002: CUED D/SOILS/TR321 White 2002 ________________________________________________________________________________________________________. 24. sample after each addition of fine material revealed that an evolution of a ‘tail’ in the.

12 Sep 2002: A A = {2, 3, 4, 5, 6, 7, 8, 10, 13, 24, 25, 27, 29, 30, 31, 33, 35, 46, 52, 58}.