We use the method of self-adjoint extensions to define a self-adjoint
operator A(T) as the singular perturbation of a given self-adjoint ope
rator A by a singular operator T on a Hilbert space. We also find the
structure of a singular operator e such that the singular perturbation
of A(2) by Q satisfies (A(2))(Q) = (A(r))(2) We obtain the explicit f
orm of Q in terms of A and T. A definition of the n-th power for stric
tly positive symmetric operators is also given.