Abstract:Akhiezer Polynomials orthogonal on several intervals are used to define a generalization of the beta integral where the integral is over two disjoint intervals of the real line, [−1, −β] ∪ [β, 1]. An explicit evaluation of the integral is given in the limiting case as β → 1.
“…In this situation we will hope to evaluate the moment integrals in terms of the parameters α and β. Owing to the nature of the set, it seems that the combination of the α and β that will replace the parameter b will be related to the gamma points for the set E. For a definition and discussion of the gamma points associated with a union of disjoint intervals see [2]. Finally, it is interesting to note that if we substitute b = 1 into the series (2.4) we should obtain a series expansion for the limiting case as b → 1 − that was calculated in [4]. The resultant identity in this case is just a special case of a hypergeometric summation but the relationship between different limiting values of integrals of these kinds over a general set E as the lengths of the disjoint intervals tend to zero is something that warrants further investigation.…”
Section: Discussionmentioning
confidence: 99%
“…In this paper we will give a series expansion of the generalized beta integral on two intervals that was defined in [4]. We will proceed directly with the definition of the integral since the motivation for the definition can be found in [4].…”
Section: Introductionmentioning
confidence: 99%
“…We will proceed directly with the definition of the integral since the motivation for the definition can be found in [4].…”
Section: Introductionmentioning
confidence: 99%
“…For a definition and discussion of the Akhiezer polynomials see [1,2] and [4]. It is clear that as b → 0 we obtain the classical beta integral.…”
Section: Introductionmentioning
confidence: 99%
“…It is clear that as b → 0 we obtain the classical beta integral. In [4] this integral and others related to it were evaluated in the limit as b → 1 − . In this paper we expand (1.1) in a power series in terms of the parameter b and evaluate the coefficients in terms of hypergeometric functions.…”
We give an explicit formula for the expansion coefficients of a generalized beta integral on the set [−1, −b] ∪ [b, 1] b ∈ (0, 1), in a power series in the parameter b, thus defining a generalized beta function of two complex variables.
“…In this situation we will hope to evaluate the moment integrals in terms of the parameters α and β. Owing to the nature of the set, it seems that the combination of the α and β that will replace the parameter b will be related to the gamma points for the set E. For a definition and discussion of the gamma points associated with a union of disjoint intervals see [2]. Finally, it is interesting to note that if we substitute b = 1 into the series (2.4) we should obtain a series expansion for the limiting case as b → 1 − that was calculated in [4]. The resultant identity in this case is just a special case of a hypergeometric summation but the relationship between different limiting values of integrals of these kinds over a general set E as the lengths of the disjoint intervals tend to zero is something that warrants further investigation.…”
Section: Discussionmentioning
confidence: 99%
“…In this paper we will give a series expansion of the generalized beta integral on two intervals that was defined in [4]. We will proceed directly with the definition of the integral since the motivation for the definition can be found in [4].…”
Section: Introductionmentioning
confidence: 99%
“…We will proceed directly with the definition of the integral since the motivation for the definition can be found in [4].…”
Section: Introductionmentioning
confidence: 99%
“…For a definition and discussion of the Akhiezer polynomials see [1,2] and [4]. It is clear that as b → 0 we obtain the classical beta integral.…”
Section: Introductionmentioning
confidence: 99%
“…It is clear that as b → 0 we obtain the classical beta integral. In [4] this integral and others related to it were evaluated in the limit as b → 1 − . In this paper we expand (1.1) in a power series in terms of the parameter b and evaluate the coefficients in terms of hypergeometric functions.…”
We give an explicit formula for the expansion coefficients of a generalized beta integral on the set [−1, −b] ∪ [b, 1] b ∈ (0, 1), in a power series in the parameter b, thus defining a generalized beta function of two complex variables.
Moment evaluations are important for the study of non-classical orthogonal polynomial systems for which explicit representations are not known. In this paper we compute, in terms of the hypergeometric function, the moments associated with a generalized ultraspherical weight on a collection of intervals with two symmetric gaps. These moments, parametrized by the endpoints of the gaps, are identified as a one parameter deformation between the full range ultraspherical moments and the half range ultraspherical moments.
In recent years much attention has been given to Newton series representations of a regularized Zeta function. Such representations are limited as they do not lead to a series expansion for the Zeta function that converges in the critical strip. In this paper, we define a fractional Newton series which serves as the meromorphic continuation of a classical Newton Series. We show that the Riemann Zeta function can be represented by a fractional Newton series in the critical strip. Under this representation the coefficients are given in terms of differences of the zeta function evaluated at the positive half integers instead of the usual situation of evaluating at the integers. Using the method of stationary phase, we derive an asymptotic formula for these zeta differences.
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