scholarly journals Higher order Riesz transforms for Laguerre expansions

2011 ◽  
Vol 55 (1) ◽  
pp. 27-68 ◽  
Author(s):  
Jorge J. Betancor ◽  
Juan C. Fariña ◽  
Lourdes Rodríguez-Mesa ◽  
Alejandro Sanabria-García
2005 ◽  
Vol 84 (3) ◽  
pp. 375-405 ◽  
Author(s):  
Piotr Graczyk ◽  
Jean-J. Loeb ◽  
Iris A. López P. ◽  
Adam Nowak ◽  
Wilfredo O. Urbina R.

2017 ◽  
Vol 49 (3) ◽  
pp. 381-410
Author(s):  
Qingquan Deng ◽  
Yong Ding ◽  
Xiaohua Yao

2008 ◽  
Vol 46 (2) ◽  
pp. 219-250 ◽  
Author(s):  
Jorge J. Betancor ◽  
Juan C. Fariña ◽  
Teresa Martinez ◽  
Lourdes Rodríguez-Mesa

2006 ◽  
Vol 55 (3) ◽  
pp. 999-1014 ◽  
Author(s):  
E. Harboure ◽  
B. Viviani ◽  
J. L. Torrea

Author(s):  
Adam Nowak ◽  
Krzysztof Stempak

We establish a symmetrization procedure in the context of general orthogonal expansions associated with a second-order differential operator L, a Laplacian. Combining with a unified conjugacy scheme from an earlier paper by Nowak and Stempak permits, using a suitable embedding, a differential-difference Laplacian $\mathbb{L}$ to be associated with the initially given orthogonal system of eigenfunctions of L, so that the resulting extended conjugacy scheme has the natural classical shape. This means, in particular, that the related partial derivatives decomposing $\mathbb{L}$ are skew-symmetric in an appropriate L2 space and they commute with Riesz transforms and conjugate Poisson integrals. The results also shed new light on the issue of defining higher-order Riesz transforms for general orthogonal expansions.


2021 ◽  
Vol 2021 ◽  
pp. 1-28
Author(s):  
Jorge J. Betancor ◽  
Lourdes Rodríguez-Mesa

In this paper, we study higher-order Riesz transforms associated with the inverse Gaussian measure given by π n / 2 e x 2 d x on ℝ n . We establish L p ℝ n , e x 2 d x -boundedness properties and obtain representations as principal values singular integrals for the higher-order Riesz transforms. New characterizations of the Banach spaces having the UMD property by means of the Riesz transforms and imaginary powers of the operator involved in the inverse Gaussian setting are given.


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