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16 Nov 2012: Now calculate the Taylor series for f (z) aboutz = i and determine the new radius of convergence.

28 Feb 2012: However, contemporary physicsresearch leads to a number of new and important computational challenges. ... Davis, P. J. & Rabinowitz, P. (1975), Methods of Numerical Integration, AcademicPress, New York.

5 Sep 2012: Some discussion and a numerical experiment areaccordingly carried out for the new Dirichlet approximation. ... Theorem 7.2. Denoting the truncation of the new Dirichlet series (30) by.

22 Mar 2012: N. G. De Bruijn, Asymptotic Methods in Analysis, Dover Publications Inc., New York,1981. ... 535–562. 22. F. W. J. Olver, Asymptotics and special functions, in Computer Science and AppliedMathematics, Academic Press, New York, London, 1974.

22 Mar 2012: Numerical Mathe-matics and Scientific Computation. Clarendon, Oxford University Press, New York (1995). ... Dover, New York (2001)32. Vandewalle, S.: Parallel Multigrid Waveform Relaxation for Parabolic Problems.

2 Aug 2012: Φ′(Q)T p = q, suchthat K1 depends only on the new momenta. ... εH1 δ < 0,. consequently H0 pt > 0, and the new Hamiltonian to consider is.

28 Feb 2012: 252). However, both its role in deriving the dns and its representation as theproduct S1T are new. ... Chihara, T. S. (1978), An Introduction to Orthogonal Polynomials, Gordon & Breach,New York.

25 Mar 2012: Furthermore, a new violation of aconstraint can be avoided by including the constraint explicitly in the definition ofthe current X. ... O.L. Mangasarian, R.R. Meyerand S.M. Robinson, Academic Press (New York), pp.

28 Feb 2012: References. Chihara, T. S. (1978), An Introduction to Orthogonal Polynomials, Gordon & Breach,New York. ... Rainville, E. D. (1960), Special Functions, Macmillan, New York. Simon, B.

28 Feb 2012: 67, 1577–1590. Rainville, E. D. (1960), Special Functions, Macmillan, New York.

16 Jul 2012: J Reine Angew Math 458:118 5. [7] Bouchitté G, Buttazzo G (1990) New lower semicontinuity results for nonconvex functionalsdefined on measures.

16 Jul 2012: R1 = 12W[1] = 12τω. 12x 124τ. 3ω(xV )2. from W[1].Although the new W [1] and W[1] are more complicated, the computations are now.

20 Oct 2012: To overcome the issues inherent to consistent reconstructions the new approach of generalized sam-pling was introduced in [1, 4, 5]. ... Our main result in this section is to present new, sharp bounds.We first require the following lemma:.

3 Sep 2012: On optimal wavelet reconstructions from Fourier samples:linearity and universality of the stable sampling rate. B. Adcocka, A. C. Hansenb,c, and C. Poonb. aDepartment of Mathematics, Purdue UniversitybDepartment of Applied Mathematics and