Dunkl operator explained

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 kv an arbitrary "multiplicity" function on R (so ku = kv whenever the reflections σu and σv corresponding to the roots u and v are conjugate in G). Then, the Dunkl operator is defined by:

Tif(x)=

\partial
\partialxi

f(x)+

\sum
v\inR+

kv

f(x)-f(x\sigmav)
\left\langlex,v\right\rangle

vi

where

vi

is the i-th component of v, 1 ≤ iN, x in RN, and f a smooth function on RN.

Dunkl operators were introduced by . One of Dunkl's major results was that Dunkl operators "commute," that is, they satisfy

Ti(Tjf(x))=Tj(Tif(x))

just as partial derivatives do. Thus Dunkl operators represent a meaningful generalization of partial derivatives