Abstract. We provide a simple recipe for obtaining all self-adjoint extensions, together with their resolvent, of the symmetric operator S obtained by restricting the self-adjoint operator A : D (A) ⊆ H → H to the dense, closed with respect to the graph norm, subspace N ⊂ D (A) . Neither the knowledge of S * nor of the deficiency spaces of S is required. Typically A is a differential operator and N is the kernel of some trace (restriction) operator along a null subset. We parametrise the extensions by the bundle p : E(h) → P(h) , where P(h) denotes the set of orthogonal projections in the Hilbert space h D (A)/N and p −1 (Π) is the set of self-adjoint operators in the range of Π . The set of self-adjoint operators in h , i.e. p −1 (1) , parametrises the relatively prime extensions. Any (Π, Θ) ∈ E(h) determines a boundary condition in the domain of the corresponding extension A Π,Θ and explicitly appears in the formula for the resolvent (−A Π,Θ + z) −1 . The connection with both von Neumann's and Boundary Triples theories of self-adjoint extensions is explained. Some examples related to quantum graphs, to Schrödinger operators with point interactions and to elliptic boundary value problems are given.Mathematics subject classification (2000): 47B25, 47B38, 35J25.