Results 11 to 20 of about 1,259 (74)

Construction of the Shifted Modified Gegenbauer Polynomials and Approximation

open access: yesAdvances in Mathematical Physics
MSC2020 Classification: 42C05 ...
Abdelhamid Rehouma, Hossein Jafari
doaj   +2 more sources

A semicircle law and decorrelation phenomena for iterated Kolmogorov loops

open access: yesJournal of the London Mathematical Society, Volume 103, Issue 2, Page 558-586, March 2021., 2021
Abstract We consider a standard one‐dimensional Brownian motion on the time interval [0,1] conditioned to have vanishing iterated time integrals up to order N. We show that the resulting processes can be expressed explicitly in terms of shifted Legendre polynomials and the original Brownian motion, and we use these representations to prove that the ...
Karen Habermann
wiley   +1 more source

Avoiding maximal parabolic subgroups of S_k [PDF]

open access: yes, 2000
We find an explicit expression for the generating function of the number of permutations in S_n avoiding a subgroup of S_k generated by all but one simple transpositions.
Mansour, Toufik, Vainshtein, Alek
core   +4 more sources

Some results on a generalized ω‐Jacobi transform

open access: yesInternational Journal of Mathematics and Mathematical Sciences, Volume 2004, Issue 63, Page 3379-3387, 2004., 2004
We introduce a generalized ω‐Jacobi transform and obtain images of certain functions under this transform. Moreover, we define a new probability density function (pdf) involving this new generalized ω‐Jacobi function. Some basic functions associated with the pdf, such as characteristic function, moments and distribution function, are evaluated.
Y. Ben Nakhi, S. L. Kalla
wiley   +1 more source

The finite Fourier transform of classical polynomials [PDF]

open access: yes, 2014
The finite Fourier transform of a family of orthogonal polynomials $A_{n}(x)$, is the usual transform of the polynomial extended by $0$ outside their natural domain.
Dixit, Atul   +3 more
core   +3 more sources

On the Krall‐type polynomials

open access: yesJournal of Applied Mathematics, Volume 2004, Issue 5, Page 359-369, 2004., 2004
Using a general and simple algebraic approach, some results on Krall‐type orthogonal polynomials and some of their extensions are obtained.
R. Álvarez-Nodarse   +2 more
wiley   +1 more source

The second‐order self‐associated orthogonal sequences

open access: yesJournal of Applied Mathematics, Volume 2004, Issue 2, Page 137-167, 2004., 2004
The aim of this work is to describe the orthogonal polynomials sequences which are identical to their second associated sequence. The resulting polynomials are semiclassical of class s ≤ 3. The characteristic elements of the structure relation and of the second‐order differential equation are given explicitly.
P. Maroni, M. Ihsen Tounsi
wiley   +1 more source

The Hermite polynomials and the Bessel functions from a general point of view

open access: yesInternational Journal of Mathematics and Mathematical Sciences, Volume 2003, Issue 57, Page 3633-3642, 2003., 2003
We introduce new families of Hermite polynomials and of Bessel functions from a point of view involving the use of nonexponential generating functions. We study their relevant recurrence relations and show that they satisfy differential‐difference equations which are isospectral to those of the ordinary case.
G. Dattoli   +2 more
wiley   +1 more source

On a generalized Jacobi transform

open access: yesInternational Journal of Stochastic Analysis, Volume 15, Issue 4, Page 371-385, 2002., 2002
In this paper, we study a generalized Jacobi transform and obtain images of certain functions under this transform. Furthermore, we define a Jacobi random variable and derive its moments, distribution function, and characteristic function.
José Sarabia, S. L. Kalla
wiley   +1 more source

Quasi‐definiteness of generalized Uvarov transforms of moment functionals

open access: yesJournal of Applied Mathematics, Volume 1, Issue 2, Page 69-90, 2001., 2001
When σ is a quasi‐definite moment functional with the monic orthogonal polynomial system {P n (x)}n=0∞, we consider a point masses perturbation τ of σ given by τ:=σ+λΣl=1 mΣk=0 ml((−1)kulk/k!)δ (k)(x − c l), where λ, ulk, and cl are constants with ci ≠ cj for i ≠ j. That is, τ is a generalized Uvarov transform of σ satisfying A(x) τ = A(x) σ, where A(x)
D. H. Kim, K. H. Kwon
wiley   +1 more source

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