On the connection between the Fueter-Sce-Qian theorem and the generalized CK-extension

TL;DR

This paper links the Fueter-Sce-Qian theorem with the generalized CK-extension, providing explicit formulas and decompositions that enable new extensions of the Coherent State Transform in Clifford analysis.

Contribution

It offers an alternative description of the Fueter-Sce-Qian theorem via the generalized CK-extension, establishing a bijection between axial monogenic functions and real analytic functions, and introduces an axial CST.

Findings

Explicit formulas for Fueter-Sce-Qian map in even and odd dimensions

Plane wave and Radon transform decompositions of the map

Construction of an axial Coherent State Transform

Abstract

The Fueter-Sce-Qian theorem provides a way of inducing axial monogenic functions in $\mathbb{R}^{m+1}$ from holomorphic intrinsic functions of one complex variable. This result was initially proved by Fueter and Sce for the cases where the dimension $m$ is odd using pointwise differentiation, while the extension to the cases where $m$ is even was proved by Qian using the corresponding Fourier multipliers. In this paper, we provide an alternative description of the Fueter-Sce-Qian theorem in terms of the generalized CK-extension. The latter characterizes axial null solutions of the Cauchy-Riemann operator in $\mathbb{R}^{m+1}$ in terms of their restrictions to the real line. This leads to a one-to-one correspondence between the space of axially monogenic functions in $\mathbb{R}^{m+1}$ and the space of analytic functions of one real variable. We provide explicit expressions for the Fueter-Sce-Qian map in terms of the generalized CK-extension for both cases, $m$ even and $m$ odd. These expressions allow for a plane wave decomposition of the Fueter-Sce-Qian map or, more in particular, a factorization of this mapping in terms of the dual Radon transform. In turn, this decomposition provides a new possibility for extending the Coherent State Transform (CST) to Clifford Analysis. In particular, we construct an axial CST defined through the Fueter-Sce-Qian mapping, and show how it is related to the axial and slice CSTs already studied in the literature.