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Lect24.dvi
www.damtp.cam.ac.uk/user/na/PartII/Lect24.pdf4 Mar 2005: t3). (5.16). Thus,etBetC = et(BC) t 0 only if B andC commute.[Note: It is trivial to prove that commutativityis sufficient, not just necessary.]The good news is, however, -
Lect17.dvi
www.damtp.cam.ac.uk/user/na/PartII/Lect17.pdf21 Feb 2005: to the grid) pass unnoticed!Bad news:For |θ|, |ψ| = O. (. ... small attenuation already familiar from the analysis of Gauss–Seidel.Good news:Consider just thelarge frequencies.Then. -
Examples2.dvi
www.damtp.cam.ac.uk/user/na/PartII/Examples2.pdf7 Feb 2005: . . You should find that the(2, 3) element of the new matrix isO(. ... ε3). and that the new matrix has exactly thesame trace asA. -
Lect10.dvi
www.damtp.cam.ac.uk/user/na/PartII/Lect10.pdf7 Feb 2005: Definition 3.10 (Multistep methods)It is often useful to use past solution values in computing a new value.Thus, assuming thatyn, yn1,. , -
Lect07.dvi
www.damtp.cam.ac.uk/user/na/PartII/Lect07.pdf31 Jan 2005: adjacent columns of a matrix, thetotal number of nonzero elements in the new combination of rows or columns is at most five. -
Lect03.dvi
www.damtp.cam.ac.uk/user/na/PartII/Lect03.pdf19 Jan 2005: It follows from the symmetry ofAand the new assertion(2) that the proof is complete. -
Lect05.dvi
www.damtp.cam.ac.uk/user/na/PartII/Lect05.pdf25 Jan 2005: The reason for the new step2 is thatf (λ) = 0 implies thatx(k) satisfiesAx(k) = (λ s(k))x(k). -
Explicit Magnus expansions for nonlinear equations Fernando Casasa…
www.damtp.cam.ac.uk/user/na/NA_papers/NA2005_05.pdf15 Aug 2005: conveniently modified version of the Magnus expansion to construct a new class of. ... Here new Lie group solvers up to order four for (2) are presented. -
Moment-free numerical integration of highly oscillatory functions…
www.damtp.cam.ac.uk/user/na/NA_papers/NA2005_04.pdf14 Sep 2005: ωs1. ). Like the Filon-type method, this new method uses interior points as. ... A[. ddx. fg′. ]. Hence we have derived a new approximation of I[f], namely QA[f] 1iωQ. -
IserlesNorsett4.dvi
www.damtp.cam.ac.uk/user/na/NA_papers/NA2005_08.pdf23 Nov 2005: Even then the singularity of h. (with the new definition of f̃) at ξ is not removable. -
Paper.dvi
www.damtp.cam.ac.uk/user/na/NA_papers/NA2005_06.pdf21 Sep 2005: This results in a new system,. di. dxiL[v](ck) =. di. dxif(ck), i = 1, 2,. ... W. J. (1974), Asymptotics and Special Functions, Academic Press, New. York.Olver, S. -
Paper1.dvi
www.damtp.cam.ac.uk/user/na/NA_papers/NA2005_01.pdf29 Jan 2005: We now remove the bottom row of R and denote the new matrix by R̃. ... S. (1994), Introduction to Mechanics and Symmetry,Springer-Verlag, New York. Olver, P. -
Interlacing property for B-splines Simon Foucart Department of…
www.damtp.cam.ac.uk/user/na/NA_papers/NA2005_03.pdf24 Feb 2005: Proposition 11 is of particular importance for our purpose andseems to be new. ... Springer–Verlag, 1989. [11] K. Scherer and A. Shadrin. New upper bound for the B-spline basis conditionnumber. -
On the quadrature of multivariate highly oscillatory integrals over…
www.damtp.cam.ac.uk/user/na/NA_papers/NA2005_07.pdf3 Oct 2005: Academic Press, New York, NY. Olver, S. (2005). Moment-free numerical integration of highly oscillatory functions. ... Rudin, W. (1964). Principles of Mathematical Analysis. McGraw-Hill, Inc., New York, NY. -
On the value of the max-norm of the orthogonal ...
www.damtp.cam.ac.uk/user/na/NA_papers/NA2005_09.pdf14 Dec 2005: Therefore, in order to get closer to the value 2k 1, it is necessary to proposea new approach. ... Jacobi projections in: Approximation theory and applications (ZviZiegler, ed.), Academic Press, New York, 1981, 187–200. -
IserlesNorsett3.dvi
www.damtp.cam.ac.uk/user/na/NA_papers/NA2005_02.pdf17 Feb 2005: Quadrature methods for multivariate highly. oscillatory integrals using derivatives. Arieh Iserles and Syvert P. Nørsett†. We dedicate this paper to the memory of Germund Dahlquist. Abstract. While there exist effective methods for univariate -
an2000.dvi
www.damtp.cam.ac.uk/user/na/NA_papers/NA2000_03.pdf26 Sep 2005: A familiar case in pointis the discovery of solitons in the solution of the Korteweg–de Vries equation byZabusky and Kruskal (1965), an event which launched a whole new mathematicaldiscipline, other
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