Abstract

We say that a function $\alpha(x)$ belongs to the set ${\bf A}^{(\gamma)}$ if it has an asymptotic expansion of the form $\alpha(x)\sim \sum^\infty_{i=0}\alpha_ix^{\gamma-i}$ as $x\to\infty$, which can be differentiated term by term infinitely many times. A function  $f(x)$ is in the class ${\bf B}^{(m)}$ if it satisfies a linear homogeneous differential equation of the form $f(x)=\sum^m_{k=1}p_k(x)f^{(k)}(x)$, with $p_k\in {\bf A}^{(i_k)}$, $i_k$ being integers satisfying $i_k\leq k$. These functions appear in many problems of applied mathematics and other scientific disciplines. They have been shown to have many interesting properties,  and their integrals $\int^\infty_0 f(x)\,dx$, whether convergent or divergent,  can be evaluated very efficiently via the Levin--Sidi $D^{(m)}$-transformation,  a most effective convergence acceleration method. (In case of divergence, these integrals  are defined in some summability sense, such as Abel summability or Hadamard finite part or a mixture of these two.) In this note, we show that if $f(x)$ is in ${\bf B}^{(m)}$, then so is $(f\circ g)(x)=f(g(x))$, where $g(x)>0$ for all large $x$ and $g\in {\bf A}^{(s)}$,  $s$ being a positive integer. This enlarges the scope of the $D^{(m)}$-transformation considerably to include functions of complicated arguments. We demonstrate  the validity of our result with an application of the $D^{(3)}$ transformation to two integrals $I[f]$ and $I[f\circ g]$, for some $f\in{\bf B}^{(3)}$ and $g\in{\bf A}^{(2)}$. The Fa\`{a} di Bruno formula and Bell polynomials play a central role in our study.

Highlights

  • Introduction and Main ResultTfohremD∫(0m∞)transformation f (x) dx, whose is a very effective convergence acceleration tool for computing infinite-range integrands f (x) belong to the function class B(m), m being a positive integer.integrals of the Both the D(m) transformation and the function class B(m) were introduced by (Levin & Sidi, 1981) and studied further in (Sidi, 2003, Chapter 5)

  • B(m) if it integers satisfies a satisfying ik ≤ been k. These shown to hfuavnectmioannsyaipnpteearersitninmg apnroypperrotibelse,mansdotfhaepirpilnietdegmraalsth∫e0m∞ aft(icxs) and other scientific disciplines. They have dx, whether convergent or divergent, can be evaluated very efficiently via the Levin–Sidi D(m)-transformation, a most effective convergence acceleration method. (In case of divergence, these integrals are defined in some summability sense, such as Abel summability or Hadamard finite part or a mixture of these two.) In this note, we show that if f (x) is in B(m), so is ( f ◦ g)(x) = f (g(x)), where g(x) > 0 for all large x and g ∈ A(s), s being a positive integer

  • Most special functions appearing in applied mathematics and most functions arising in different scientific and engineering disciplines belong to the sets B(m)

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Summary

Introduction and Main Result

Transformation f (x) dx, whose is a very effective convergence acceleration tool for computing infinite-range integrands f (x) belong to the function class B(m), m being a positive integer. A function α(x) belongs to the set A(γ), where γ is complex in general, if it is infinitely differentiable for all large x > 0 and has a Poincare-type asymptotic expansion of the form. It is obvious that no two functions in X(γ) have the same asymptotic expansion, since if α, β ∈ X(γ), either α ≡ β or α − β ∈ A(γ−k) strictly for some nonnegative integer k. By Remarks B1, B2, B5, and B6, it is clear that the classes B(m) contain an ever increasing number of functions with varying behavior (oscillatory or nonoscillatory or combinations of the two), and this implies that the D(m) transformation is a comprehensive convergence acceleration method with ever increasing scope. We would like to mention again that most special functions that appear in scientific and engineering applications belong to one of the classes B(m)

Main Results
Proof of Main Results
Special Cases
The Case of Arbitrary m
An Example
A Further Development
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