On the analytic continuation of functions defined by regrouped power series

1974 ◽  
Vol 15 (5) ◽  
pp. 408-412
Author(s):  
V. A. Belyaev
Keyword(s):  
Power Series ◽  
Analytic Continuation

scholarly journals Polynomially bounded multisequences and analytic continuation

1982 ◽  
Vol 23 (1) ◽  
pp. 41-52
Author(s):  
Daniel J. Troy
Keyword(s):  
Power Series ◽  
Analytic Continuation ◽  
Linear Functional ◽  
Necessary And Sufficient Condition ◽  
Convergence Criteria ◽  
Dimensional Torus ◽  
Unit Factor ◽  
Image Position ◽  
Necessary And Sufficient ◽  
Class Of Functions

Given a polynomially bounded multisequence {fm}, where m = (m1, …, mk) ∈ ℤk, we will consider 2k power series in exp(iz1), …, exp(izk), each representing a holomorphic function within its domain of convergence. We will consider this same multisequence as a linear functional on a class of functions defined on the k-dimensional torus by a Fourier series, , with the proper convergence criteria. We shall discuss the relationships that exist between the linear functional properties of the multisequence and the analytic continuation of the holomorphic functions. With this approach we show that a necessary and sufficient condition that the multisequence be given by a polynomial is that each of the power series represents, up to a unit factor, the same function that is entire in the variables

scholarly journals The a-points of Faber polynomials for a special function

1970 ◽  
Vol 11 (1) ◽  
pp. 1-6
Author(s):  
Hassoon S. Al-Amiri
Keyword(s):  
Analytic Function ◽  
Power Series ◽  
Analytic Continuation ◽  
Special Function ◽  
Laurent Expansion ◽  
Faber Polynomials ◽  
Analytic Element ◽  
Formal Expansion ◽  
Image Position

Let f(ζ) be a power series of the formwhere lim sup |an|1/n < ∞. The Faber polynomials {fn(ζ)} (n = 0, 1, 2, …) are the polynomial parts of the formal expansion of (f(ζ))n about ζ = ∞. Series (1) defines an analytic element of an analytic function which we designate as w = f(ζ). Since at ζ = ∞ the analytic element is univalent in some neighborhood of infinity; thus the inverse of this element is uniquely determined in some neighborhood of w= ∞, and has a Laurent expansion of the formwhere lim sup |bn|1/n = p < ∞. Let ζ = g(w) be this single-valued function defined by (2) in |w| > p. No analytic continuation of g(w) will be considered.

Analytic Continuation of Power Series by Regular Generalized Weighted Means

1983 ◽  
Vol 26 (4) ◽  
pp. 454-463
Author(s):  
Bruce L. R. Shawyer ◽  
Ludwig Tomm
Keyword(s):  
Analytic Function ◽  
Power Series ◽  
Analytic Continuation ◽  
Unit Disc ◽  
Meromorphic Functions ◽  
Geometric Series ◽  
Summability Methods ◽  
Weighted Means ◽  
Simply Connected Region ◽  
Simply Connected

AbstractThe behaviour of summability transforms of power series outside their circles of convergence has been studied by many authors. In the case of the geometric series Luh [6] and Tomm [10] showed that there exist regular methods A which provide an analytic continuation into any given simply connected region G that contains the unit disc but not the point 1. Moreover, the Atransforms of the geometric series may be required to converge to any chosen analytic function on prescribed regions outside the unit circle. In this paper, these results are extended to power series representing other meromorphic functions. It is also shown that the summability methods involved may be chosen to be generalized weighted means previously introduced by Faulstich [1].

A novel analytic continuation power series solution for the perturbed two-body problem

2019 ◽  
Vol 131 (10) ◽  
Author(s):  
Kevin Hernandez ◽  
Tarek A. Elgohary ◽  
James D. Turner ◽  
John L. Junkins
Keyword(s):  
Power Series ◽  
Analytic Continuation ◽  
Series Solution ◽  
Body Problem ◽  
Power Series Solution ◽  
Two Body Problem
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