~')) come from vector bundle maps E~. By 8.5, ~l(y) acts on H~,. This corresponds to an action of g-I(y) on V. (It is induced by the adjoint action of M(y) on its Lie algebra
GEORGE LUSZTIG Similarly, E; = (I, | H.~"(~,, s F, = E, |162 E;. By 8.3, the operators A(w), A(~) (resp. A'(w), A'(~)) on n.m~"(~,,.~) (resp. H.~*'(.~',,.~')) come from vector bundle maps A(w), A(~):E-+ E (resp. A'(w), A'(~):E'-~ E'), inducing the identity on the base V. Hence these operators act on each fibre E,, E~. By 8.5, ~l(y) acts on H~,,. This corresponds to an action of g-I(y) on V. (It is induced by the adjoint action of M(y) on its Lie algebra.) Moreover, E, E' are natu-rally ~I(y)-equivariant vector bundles over V and the operators A(w), A(~), A'(w), A'(~) on them are ~/(y)-invariant.