Abstract:The classical Fischer decomposition of polynomials on Euclidean space makes it possible to express any polynomial as a sum of harmonic polynomials multiplied by powers of |x| 2 . A deformation of the Laplace operator was recently introduced by Ch.F. Dunkl. It has the property that the symmetry with respect to the orthogonal group is broken to a finite subgroup generated by reflections (a Coxeter group). It was shown by B. Ørsted and S. Ben Said that there is a deformation of the Fischer decomposition for polyn… Show more
“…In fact, the relations (6) hold in any dimension and for any choice of the reflection group with different values of the constant γ [3,23]. Let P N (R 3 ) denote the space of homogeneous polynomials of degree N in R 3 , where N is a nonnegative integer.…”
Section: Laplace-and Dirac-dunkl Operators In Rmentioning
The Dirac-Dunkl operator on the 2-sphere associated to the Z 3 2 reflection group is considered. Its symmetries are found and are shown to generate the Bannai-Ito algebra. Representations of the Bannai-Ito algebra are constructed using ladder operators. Eigenfunctions of the spherical Dirac-Dunkl operator are obtained using a Cauchy-Kovalevskaia extension theorem. These eigenfunctions, which correspond to Dunkl monogenics, are seen to support finite-dimensional irreducible representations of the Bannai-Ito algebra.
“…In fact, the relations (6) hold in any dimension and for any choice of the reflection group with different values of the constant γ [3,23]. Let P N (R 3 ) denote the space of homogeneous polynomials of degree N in R 3 , where N is a nonnegative integer.…”
Section: Laplace-and Dirac-dunkl Operators In Rmentioning
The Dirac-Dunkl operator on the 2-sphere associated to the Z 3 2 reflection group is considered. Its symmetries are found and are shown to generate the Bannai-Ito algebra. Representations of the Bannai-Ito algebra are constructed using ladder operators. Eigenfunctions of the spherical Dirac-Dunkl operator are obtained using a Cauchy-Kovalevskaia extension theorem. These eigenfunctions, which correspond to Dunkl monogenics, are seen to support finite-dimensional irreducible representations of the Bannai-Ito algebra.
“…Suppose that (20) holds at level n and consider the set B = B ∪{x} with x ∈ A and |A ∩ B| = n. Consider y ∈ A ∩ B; one can write Γ B as in (18). Since x, y ∈ A, Γ A commutes with Γ {x,y} and one can write {Γ A , Γ B } as in (19), the only difference with (19) being that x, y ∈ A. Upon applying the induction hypothesis, one finds (20) with B replaced by B after a straightforward calculation.…”
Abstract. The kernel of the Z n 2 Dirac-Dunkl operator is examined. The symmetry algebra An of the associated Dirac-Dunkl equation on S n−1 is determined and is seen to correspond to a higher rank generalization of the Bannai-Ito algebra. A basis for the polynomial null-solutions of the DiracDunkl operator is constructed. The basis elements are joint eigenfunctions of a maximal commutative subalgebra of An and are given explicitly in terms of Jacobi polynomials. The symmetry algebra is shown to act irreducibly on this basis via raising/lowering operators. A scalar realization of An is proposed.
“…In fact Ker(Ds) is, as a vector space, isomorphic to P ol(R 2n+2 ) (see Corollary 5.5) and we leave the question of its representation theoretic content open. In [18], the authors studied the specific deformation of Howe duality and Fischer decomposition for the Dirac operator acting on spinor valued polynomials, coming from the Dunkl deformation of the Dirac operator. It is an interesting question to develop the Dunkl version of the symplectic Dirac operator in the context of symplectic reflection algebras (see [11]).…”
Section: Open Questions and Unresolved Problemsmentioning
We study various aspects of the metaplectic Howe duality realized by Fischer decomposition for the metaplectic representation space of polynomials on R 2n valued in the Segal-Shale-Weil representation. As a consequence, we determine symplectic monogenics, i.e. the space of polynomial solutions of the symplectic Dirac operator Ds.
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