“…We assert that L(Ax) R is dense in R. Otherwise there exists g 0 in R such that (9) fe rZg(Lu) 0 for all u coo(E) f'l A with IIAu + ull finite. In particular, (9) Thus we can expand rZg in terms of spherical harmonics in r >= a for some a" (11) rZg a,.,j(r) Ym,j(O, dp). m=Oj=-m Let h.,(r) equal "'m+4() /2(r)/ and U,j(r, 0, ) equal h(r)Y,j(O, ).…”