Researchers
Tom H. Koornwinder (University of Amsterdam) and
Marta Mazzocco (ICREA – Universitat Politècnica de Catalunya – CRM) have recently published the article
Automorphisms of the DAHA of type 
and non‑symmetric Askey–Wilson functions in
Indagationes Mathematicae. In this work, the authors
analyze the internal symmetries of double affine Hecke algebras (DAHA) and study how these symmetries act on Askey‑Wilson (AW) polynomials and functions, both in the symmetric and non‑symmetric settings.
At first glance, one expects symmetries to move neatly within the world of polynomials. But some symmetries behave like a zoom tool: once applied, the picture demands higher resolution. What looked discrete (polynomials) must be viewed in a continuous setting (functions) for the transformation to make full sense. The paper leverages this change of scale to illuminate where the natural language of DAHA symmetries truly lives.
The work focuses on the relationship between algebraic structures and special functions—fundamental objects in representation theory and mathematical analysis—with deep connections to harmonic analysis and mathematical physics.
A well‑known structure — still with unanswered questions
Double affine Hecke algebras (DAHA), introduced by Cherednik, are central in representation theory and in the study of special functions. In the rank‑one case, the DAHA of type 
is closely related to Askey–Wilson polynomials and functions, which occupy the top level of the q‑Askey scheme of orthogonal polynomials.
Previous works had identified actions of various symmetry groups—such as modular groups or Weyl‑type groups—on operators associated with the DAHA and even on the algebra itself. However, a systematic account of how these symmetries act on the relevant eigenfunctions, in particular on Askey–Wilson polynomials and functions, was still missing. In particular, it was unclear whether these symmetries preserve the polynomial world or require a broader functional framework.
Moreover, the DAHA of type is related to the Painlevé VI equation through the quantization of its monodromy group. This naturally raises the question of to what extent the classical symmetries of Painlevé VI can be lifted to the DAHA level.
Earlier work had shown that certain transitions within the q‑Askey scheme admit a geometric interpretation. For instance, the limit from Askey–Wilson polynomials to dual q‑Hahn polynomials can be viewed as the process of merging two holes on a four‑holed Riemann sphere. Choosing different pairs of holes leads to different polynomial families, such as the Big q‑Jacobi polynomials. This geometric perspective naturally raises the question of what mechanism distinguishes these choices and points toward the study of the symmetries underlying Askey–Wilson polynomials and, ultimately, the DAHA that governs them.
What happens when a symmetry changes the rules
In this work, the authors initiate a research programme aimed at studying—and potentially classifying—the symmetries of the DAHA of type and of the Zhedanov algebra, as well as understanding how the symmetries of these two structures are related and how they act on Askey–Wilson polynomials and functions.
One of the most striking results is the detailed analysis of a specific symmetry, denoted 
, which acts in a simple way on the Askey–Wilson parameters. Surprisingly, this transformation does not preserve the class of polynomials, but instead maps Askey–Wilson polynomials to Askey–Wilson functions, revealing a natural mechanism that connects these two objects and showing that the functional setting is the most appropriate one for studying certain DAHA symmetries.
In other words, the symmetry works best when you change scale: from the discrete grid of polynomials (pixels) to the continuous image of functions.
In addition, the authors propose a precise definition of the non-symmetric Askey–Wilson function in the rank‑one case, based on the Cherednik–Stokman kernel, and show that this function admits an explicit decomposition into a symmetric part and an anti-symmetric part. This decomposition allows for a clear description of its spectral properties and its behaviour under DAHA symmetries. Think of the non‑symmetric AW function like an image decomposed into two complementary color layers: warm tones (symmetric layer) and cool tones (anti‑symmetric layer). Each layer is meaningful on its own, but together they render the full picture with contrast and direction. This is exactly what the decomposition achieves: it reveals the internal structure that only becomes visible once you’ve changed scale from polynomials to functions.
Overall, the work combines techniques from algebra, analysis, and the theory of special functions, offering a unified perspective on how algebraic symmetries are reflected in concrete transformations of functions.
A wider landscape for special functions
The results of this article open several promising research directions. On the one hand, they clarify the role of DAHA automorphisms as bridges between different types of special functions, suggesting that analogous transformations may exist in higher rank or for other types of Hecke algebras.
On the other hand, the systematic study of non-symmetric Askey–Wilson functions reinforces their importance as fundamental objects, with potential applications in non-commutative harmonic analysis, representation theory, and models of mathematical physics related to quantum symmetries.
Finally, this work contributes to a deeper understanding of the q-Askey scheme and its internal symmetries, representing an important step towards a more global theory connecting orthogonal polynomials, Hecke algebras, and algebraic geometry.
Symmetry here acts like a change of scale: it asks us to move from the discrete world of polynomials to the continuous world of functions.
By shifting the focus to Askey–Wilson functions, this work shows where the natural language of DAHA symmetries truly lives.
From this unified viewpoint, new paths emerge toward deeper structures, richer connections, and future breakthroughs across mathematics and mathematical physics.
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