Let AA be a densely defined closed on a complex . Its deficiency subspaces are

N+=ker⁡(A∗−iI),N−=ker⁡(A∗+iI),\mathcal N_+=\ker(A^*-iI),\qquad \mathcal N_-=\ker(A^*+iI),

where A∗A^* is the . The deficiency indices are the cardinal dimensions

n+(A)=dim⁡N+,n−(A)=dim⁡N−.n_+(A)=\dim\mathcal N_+,\qquad n_-(A)=\dim\mathcal N_-.

They may be finite or infinite. More generally, dim⁡ker⁡(A∗−zI)\dim\ker(A^*-zI) is constant as zz ranges over either open half-plane; n+n_+ uses the upper half-plane and n−n_- the lower half-plane under the convention above.

Self-adjointness and extensions

The operator AA is exactly when n+(A)=n−(A)=0n_+(A)=n_-(A)=0. It has a on the same Hilbert space exactly when n+(A)=n−(A)n_+(A)=n_-(A); when these common dimensions are nonzero, unitary maps from N+\mathcal N_+ to N−\mathcal N_- parametrize the extensions. This is von Neumann’s extension theorem.

Closure and geometric meaning

If a symmetric operator is not closed, its deficiency indices are defined to be those of its . For a closed symmetric AA, the domain of A∗A^* decomposes into the domain of AA together with the two deficiency subspaces. The latter measure the independent boundary data missing from AA; equality of their dimensions is precisely what permits those data to be paired to form a self-adjoint domain.

Examples and sign convention

The minimal momentum operator −i d/dx-i\,d/dx on a bounded interval, obtained by closing the operator on , has deficiency indices (1,1)(1,1) and admits a circle of self-adjoint boundary conditions. On the whole real line the corresponding minimal operator has indices (0,0)(0,0) and is essentially self-adjoint. Interchanging ii and −i-i, or changing the sign of the operator, swaps the ; a source’s convention should therefore be checked before comparing formulas.

References
  1. Konrad Schmüdgen, Unbounded Self-adjoint Operators on Hilbert Space, Graduate Texts in Mathematics 265, Springer, 2012. DOI record. Relevant: Chapter 13 on deficiency indices and self-adjoint extensions.
  2. Michael Reed and Barry Simon, Methods of Modern Mathematical Physics II: Fourier Analysis, Self-Adjointness, Academic Press, 1975. Bibliographic record. Relevant: Chapter X on self-adjoint extensions.