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knowlewj01
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Homework Statement
The hamiltonian for a given interaction is
[itex] H=-\frac{\hbar \omega}{2} \hat{\sigma_y}[/itex]
where
[itex]\sigma_y = \left( \begin{array}{cc} 0 & i \\ -i & 0 \end{array} \right)[/itex]
the pauli Y matrix
Homework Equations
The Attempt at a Solution
So from the time dependant schrodinger equation we, can take the time dependence and put it into the time evolution operator U(t)
[itex]HU(t)\left|\Psi(r,0)\right>=i\hbar \frac{d}{dt}U(t)\left|\Psi(r,0)\right>[/itex]
becomes
[itex]i\hbar\frac{d}{dt}U(t) = HU(t)[/itex]
so for a non time dependant Hamiltonian H, this means:
[itex]U(t) = e^{-\frac{i}{\hbar}H t}[/itex]
so we have then:
[itex]U(t) = e^{\frac{i\omega t}{2}\hat{\sigma_y}}[/itex]
How do you treat this? Is there any particular identity that allows you to move the operator out of the exponent?
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