atyy said:
Is this an example of the difference you are talking about, or is it yet another difference?
http://mathworld.wolfram.com/BerryConjecture.html:"...physicists define this operator to be Hermitian, mathematicians do not."
Let [itex]A[/itex] be a densely defined linear operator on a Hilbert space. One of the defining properties, *, for all cases is
[tex]\left<Ax,y\right> = \left<x,Ay\right>, \ *[/tex]
where [itex]x[/itex] and [itex]y[/itex] are elements of the Hilbert space.
The text that was used for the functional analysis course that I took as a student makes the following definitions:
[itex]A[/itex] is Hermitian if [itex]A[/itex] is bounded and * is true for every [itex]x[/itex] and [itex]y[/itex] in the Hilbert space;
[itex]A[/itex] is symmetric if * holds for for every [itex]x[/itex] and [itex]y[/itex] in the domain of [itex]A[/itex];
[itex]A[/itex] is self-adjoint if [itex]A[/itex] is symmetric and the domain of [itex]A[/itex] equals the domain of [itex]A^\dagger[/itex].
According to these defintions, every Hermitian operator is and self-adjoint, but not all self-adjoint operators are Hemitian. Some books leave off the first definition and call symmetric operators Hermitian. Then, every self-adjoint operator is Hermitian, but not all Hermitian operators are self-adjoint.
MathWorld said:
Note that [itex]A[/itex] is symmetric but might have nontrivial deficiency indices, so while physicists define this operator to be Hermitian, mathematicians do not.
A symmetric (or Hemitian, depending on the terminology used) operator is self-adjoint iff it has trivial deficiency indices. Some physicists and physics references do not distinguish between the above defintions, and use the terms Hermitian and self-adjoint interchangeably to refer to all cases.
If [itex]A[/itex] is unbounded, then the Hilbert space is necessarily infinite-dimensional, and the domain of [itex]A[/itex] need not be all of the Hilbert space. If this is the case and if [itex]A[/itex] is symmetric, then the domain of [itex]A[/itex] is a subset of the domain of [itex]A^\dagger[/itex], which I have not defined.
In physics, the canonical commutation relation is important. If self-adjoint operators [itex]A[/itex] and [itex]B[/itex] satisfy such a relation, then it is easy to show that at least one of the operators must be unbounded. Suppose it is [itex]A[/itex]. The Hellinger-Toeplitz theorem states any linear operator that satisfies * for all elements of the Hilbert space must bounded. Since [itex]A[/itex] is self-adjoint and unbounded, the domain of physical observable [itex]A[/itex] cannot be all of Hilbert space!
For one consequence of these concepts, see
https://www.physicsforums.com/showthread.php?t=122063&highlight=dirac.