Symmetric operator

For physical consistency, the mean values of any dynamical variable \; \mathcal{A} must be real numbers: this implies that the mean values of the operator \; A which describes \; \mathcal{A} must be real, i.e. that : \langle \psi,A\psi \rangle= \langle \psi,A\psi\rangle^* = \langle A\psi,\psi\rangle , \quad \psi \in \mathcal{D}(A), where \; \mathcal{D}(A) is the domain of the operator \; A. It can be proved that this condition is equivalent to the following: : \langle \psi,A\chi \rangle= \langle A\psi,\chi\rangle , \quad \psi, \chi \in \mathcal{D}(A). Having defined the linear operator \; A^\dagger in \; \mathcal{H}, which is called the ''adjoint'' of \; A, such that : \langle A^\dagger\psi,\chi \rangle= \langle \psi,A\chi\rangle , \quad \psi, \chi \in \mathcal{H}, it follows that \; A must be ''Hermitian'', i.e. its domain must be such that \; \mathcal{D}(A) \subseteq \mathcal{D}(A^\dagger) and \; A must coincide with \; A^\dagger in \; \mathcal{D}(A). '''Definition: Hermitian [[operators]] whose domain is dense in \; \mathcal{H} are called '''symmetric'''.''' In particular, if a ''bounded'' linear operator is symmetric, it is also a Hermitian and [[self-adjoint operator]]. {{stub}} [[Category:Mathematical Structure]] [[Category:Handbook of Quantum Information]]