ABSTRACT
REMARKS. (1) In the next chapter we shall sec that in the case dim(X) = d0 = I (for \Vhich F is necessarily reduced to (X, r) where r is
In this context, one can be much more precise about the constant KF appearing in the main theorem 4. Optimal results in this situation can be stated as follows. Theorem 5. If dirnX = 2, the weighted energy representation is irreducible if any root a of g satisfies
