Search

31 Dec 2007: If the. higher value, from CDF, should turn out to be correct, this is a clear signal that some new.

11 Apr 2007: 2Q(new) 2Q(old) = m1i=1 µi (xi x0) (xi x0)T , (17). ... 2Q(new) 2F ‖2F = ‖2Q(old) 2F ‖2F ‖2Q(new) 2Q(old)‖2F , (18).

25 Jan 2007: P = (η1 η2 η3) matrix with columns components of new basis vectors ηk. ... Hence use this new scalar product as a definition of length or norm:.

30 Mar 2007: The new sine terms sk, unlike the standard Fourier series sine terms dk, also decay like O(k2. ). ... irregular oscillations, Math. Comp. 38 (1982), no. 158 531–538.[8] Olver, F.W.J., Asymptotics and Special Functions, Academic Press, New York, 1974.

21 Nov 2007: The given conclusions may assistthe development of some new software for unconstrained optimization. ... A report on theprogress so far of this new work is given in the next section.

25 Jan 2007: errata and new note sets. ... Then we have new inertial co-ordinates. t′ = γ(v)(t vx)x′ = γ(v)(x vt)y′ = y.

7 Aug 2007: S. Leite, and J. Jakubiak. A new geometric algorithm to gener-ate smooth interpolating curves on Riemannian manifolds.

19 Oct 2007: Kantorovich, L. V. & Krylov, V. I. (1958),Approximate Methods of Higher Analysis, 3rd edn,Interscience, New York. ... NA2007/02. Rainville, E. D. (1960),Special Functions, Macmillan, New York. Roache, P.

25 Jan 2007: Replace x by the new variable ξ = x p21t. Then η1 is. ... Replace x by the new variable ξ = x p22t. Then η2 is constant and.

25 Jan 2007: Recently an outstanding new textbook book came out which I strongly rec-ommend for the physical side of GR. ... This allows us to pass to a new(non-inertial) coordinate system. x̃ = x b(t), (17).