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Wilson's functional equation on C
Authors:Henrik Stetkaer
Institution:(1) Department of Mathematics, Aarhus University, Ny Munkegade, DK-8000 Aarhus C, Denmark
Abstract:Summary We find the complete set of continuous solutionsf, g of ldquoWilson's functional equationrdquoSgr n = 0 N – 1 f(x + wny) = Nf(x)g(y), x, y isin C, given a primitiveN th rootw of unity.Disregarding the trivial solutionf = 0 andg any complex function, it is known thatg satisfies a version of d'Alembert's functional equation and so has the formg(z) = g epsi(z) = N–1 Sgr n = 0 N – 1 Emgr(wnz) for somemgr isin C2. HereE (mgr1, mgr2)(x + iy) = exp(mgr 1x + mgr2).For fixedg = g mgr the space of solutionsf of Wilson's functional equation can be decomposed into theN isotypic subspaces for the action of Z N on the continuous functions on C. We prove that ther th component, wherer isin {0, 1, ctdot,N – 1}, of any solution satisfies the signed functional equationSgr n = 0 N – 1 f(x + wny)wnr = Ng(x)f(y), x, y isin C. We compute the solution spaces of each of these signed equations: They are 1-dimensional and spanned byz rarr Sgr n = 0 N – 1 wnr Emgr(wnz), except forg = 1 andr ne 0 where they are spanned by 
$$\bar z^r $$
andz N – r. Adding the components we get the solution of Wilson's equation. Analogous results are obtained with the action ofZ N on C replaced by that ofSO(2).The case ofg = 0 in the signed equations is special and solved separately both for Z N andSO(2).
Keywords:39B32
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