Expectation formula in Dirac notation.

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\langle \hat{A} \rangle = \langle x|\hat{A}|x \rangle = \int \psi_{x}^{"*"} \hat{A} \psi_{x} \,d \tau

This is the expectation value postulate of quantum mechanics.

If the wavefunction \psi_{x} is not an eigenfunction of the operator \hat{A} then the measured value of the observable A is variable. When \psi_{x} is normalized such that
\int \psi_{x}^{"*"}\psi_{x} \,d \tau=1
the expectation value above yeilds the average measurement of all possible measurements of A. (Note that d \tau indicates an integration over all space.) This works because, since \hat{A} is an Hermitian operator, its eigenvectors form an orthonormal basis. It follows that any function can be written as an infinite linear combination of eigenfunctions of \hat{A}.
 
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Time reversal invariant Hamiltonians must satisfy ##[H,\Theta]=0## where ##\Theta## is time reversal operator. However, in some texts (for example see Many-body Quantum Theory in Condensed Matter Physics an introduction, HENRIK BRUUS and KARSTEN FLENSBERG, Corrected version: 14 January 2016, section 7.1.4) the time reversal invariant condition is introduced as ##H=H^*##. How these two conditions are identical?

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