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There is a theory of spherical harmonics for measures invariant under a finite reflection group. The measures are products of powers of linear functions, whose zero-sets are the mirrors of the reflections in the group, times the rotation-invariant measure on the unit sphere in R n { {R}ⁿ}. A commutative set of differential-difference operators, each homogeneous of degree − 1 -1, is the analogue of the set of first-order partial derivatives in the ordinary theory of spherical harmonics. In the case of R 2 { {R}²} and dihedral groups there are analogues of the Cauchy-Riemann equations which apply to Gegenbauer and Jacobi polynomial expansions.
Charles F. Dunkl (Sun,) studied this question.