For physical consistency, the mean values of any dynamical variable must be real numbers: this implies that the mean values of the operator which describes must be real, i.e. that
:
where is the domain of the operator .
It can be proved that this condition is equivalent to the following:
:.
Having defined the linear operator in , which is called the ''adjoint'' of , such that
:,
it follows that must be ''Hermitian'', i.e. its domain must be such that and must coincide with in .
'''Definition:
Hermitian [[operators]] whose domain is dense in are called '''symmetric'''.'''
In particular, if a ''bounded'' linear operator is symmetric, it is also a Hermitian and [[self-adjoint operator]].
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[[Category:Mathematical Structure]]
[[Category:Handbook of Quantum Information]]