“…For 1 2 < s < n 2 − p one of these representations is the corresponding complementary series representation of O(1, n) onḢ s− 1 2 ,p (R n−1 ), and the restriction mapḢ s,p (R n ) →Ḣ s− 1 2 ,p (R n−1 ) projects onto this component. This observation makes it possible to use the machinery of symmetry breaking operators whose study was recently initiated by Kobayashi [6] (see also [4,7,8,9]). In this language the differential operator ∆ a,p (a = 2(1 − s)) corresponds to the action of the Casimir element of O(1, n) inḢ s,p (R n ) and the fractional Branson-Gover operators are the standard Knapp-Stein intertwining operators between principal series representations of the group O(1, n).…”