The time evolution operator (QM) Algebraic properties

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Homework Statement



The hamiltonian for a given interaction is

H=-\frac{\hbar \omega}{2} \hat{\sigma_y}

where

\sigma_y = \left( \begin{array}{cc} 0 & i \\ -i & 0 \end{array} \right)

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)

HU(t)\left|\Psi(r,0)\right>=i\hbar \frac{d}{dt}U(t)\left|\Psi(r,0)\right>

becomes

i\hbar\frac{d}{dt}U(t) = HU(t)

so for a non time dependant Hamiltonian H, this means:

U(t) = e^{-\frac{i}{\hbar}H t}

so we have then:

U(t) = e^{\frac{i\omega t}{2}\hat{\sigma_y}}

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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edit: changed the matrix to the correct form
 
Do you know how the exponential of a finite matrix is defined? If so, use the definition.
 
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