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Frank Stenger

Publications and source records attributed to Frank Stenger.

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Indefinite Integration Operators Identities and their Approximations

The integration operators (*) $({\mathcal J}^+\,g)(x) = \int_a^x g(t) \, dt$ and (**) $({\mathcal J}^-\,g)(x) = \int_x^b g(t) \, dt$ defined on an interval $(a,b) \subseteq {\mathbf R}$ yield new identities for indefinite convolutions, control theory, Laplace and Fourier transform inversion, solution of differential equations, and solution of the classical Wiener--Hopf integral equations. These identities are are expressed in terms of ${\mathcal J}^\pm$\, and they are thus esoteric. However the integrals (*) and (**) can be approximated in many ways, yielding novel and very accurate methods of approximating all of the above listed relations. Several examples are presented, mainly using Legendre polynomial as approximations, and references are given for approximation of some of the operations using Sinc methods. These examples illustrate for a class of sampled statistical models, the possibility of reconstructing models much more efficiently than by the usual slow Monte--Carlo $({\mathcal O}(N^{-1/2})$ rate. Our examples illustrate that we need only sample at $5$ points to get a representation of a model that is uniformly accurate to nearly $3$ significant figure accuracy.

math.NA

All Zeros of the Riemann Zeta Function in the Critical Strip are Located on the Critical Line and are Simple

In this paper we study the function G(z) := int{0,infinity} y^{z-1}(1 + \exp(y))^{-1} dy, for z in C. We derive a functional equation that relates G(z) and G(1 - z) for all z in C, and we prove: -- That G and the Riemann Zeta function Zeta have exactly the same zeros in the critical region D := z in C: Re z in (0,1); -- All the zeros of the Riemann Zeta function located on the critical line are simple; and -- The Riemann hypothesis, i.e., that all of the zeros of G in D are located on the critical line L := {z in D : Re z = 1/2}.

math.GM