Dunkl operator

Short description: Mathematical operator

In mathematics, particularly the study of Lie groups, a Dunkl operator is a certain kind of mathematical operator, involving differential operators but also reflections in an underlying space.

Formally, let G be a Coxeter group with reduced root system R and k_v an arbitrary "multiplicity" function on R (so k_u = k_v whenever the reflections σ_u and σ_v corresponding to the roots u and v are conjugate in G). Then, the Dunkl operator is defined by:

[math]\displaystyle{ T_i f(x) = \frac{\partial}{\partial x_i} f(x) + \sum_{v\in R_+} k_v \frac{f(x) - f(x \sigma_v)}{\left\langle x, v\right\rangle} v_i }[/math]

where [math]\displaystyle{ v_i }[/math] is the i-th component of v, 1 ≤ i ≤ N, x in R^N, and f a smooth function on R^N.

Dunkl operators were introduced by Charles Dunkl (1989). One of Dunkl's major results was that Dunkl operators "commute," that is, they satisfy [math]\displaystyle{ T_i (T_j f(x)) = T_j (T_i f(x)) }[/math] just as partial derivatives do. Thus Dunkl operators represent a meaningful generalization of partial derivatives.

References

• Dunkl, Charles F. (1989), "Differential-difference operators associated to reflection groups", Transactions of the American Mathematical Society 311 (1): 167–183, doi:10.2307/2001022, ISSN 0002-9947