Determinantal representations for the J transformation

Abstract

The iterative J transformation [Homeier, H. H. H. (1993): Some applications of nonlinear convergence accelerators. Int. J. Quantum Chem. 45, 545-562] is of similar generality as the well-known E algorithm [Brezinski, C. (1980): A general extrapolation algorithm. Numer. Math. 35, 175-180. Hâvie, T. (1979): Generalized Neville type extrapolation schemes. BIT 19, 204-213]. The properties of the J transformation were studied recently in two companion papers [Homeier, H. H. H. (1994a): A hierarchically consistent, iterative sequence transformation. Numer. Algo. 8, 47-81. Homeier, H. H. H. (1994b): Analytical and numerical studies of the convergence behavior of the J transformation. J. Comput. Appl. Math., to appear]. In the present contribution, explicit determinantal representations for this sequence transformation are derived. The relation to the Brezinski-Walz theory [Brezinski, C., Walz, G. (1991): Sequences of transformations and triangular recursion schemes, with applications in numerical analysis. J. Comput. Appl. Math. 34, 361-383] is discussed. Overholt's process [Overholt, K. J. (1965): Extended Aitken acceleration. BIT 5, 122-132] is shown to be a special case of the J transformation. Consequently, explicit determinantal representations of Overholt's process are derived which do not depend on lower order transforms. Also, families of sequences are given for which Overholt's process is exact. As a numerical example, the Euler series is summed using the J transformation. The results indicate that the J transformation is a very powerful numerical tool.