Half Spin in QM: Calculating Probability of Measured Eigenvalue at Time T=2T

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Problem:
a half spin has an eigenstate of the opertaor S_x (which is defined by the multiplication of half h bar times pauli sigma x matrix) of eigen value + half h bar at time t=0.
the spin is at a magnetic field (0,0,B) which correspond to the hamiltonian H=w(B)\hbar*\sigma_z, at time T they change the direction of the magnetic field to the y direction: (0,B,0), after another time T a measurement of S_x was done, what is the probability that the value measured is the one we started with?

My answer:
now from 0<t<T we have that |\psi(t)&gt;=e^{-iHt/\hbar}|\psi(0)&gt;
which equals: |\psi(t)&gt;=\frac{1}{\sqrt 2}(cos(wt)-isin(wt),cos(wt)+isin(wt))
now from T to 2T we have a magnetic field working in the y direction, does it mean we should act the above operator on |psi(T)> but with the appropiate change i.e should it be soemthing like this, at time t=T, |psi(T)&gt;=\frac{1}{\sqrt 2}(cos(wT)-isin(wT),cos(wT)+isin(wT)), now in order to find |psi(t)> at [T,2T] should it be:
|\psi(t)&gt;=e^{-iw(B)\hbar \sigma_y(t-T)/\hbar}|\psi(T)&gt; or something else?
from there in order to calculate the wanted probability i need to compute:
||&lt;\psi(0)|\psi(2T)&gt;|^2
is my approach correct or does it have loopholes?

any input?
thanks in advance.
 
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anyone?
if someone already asked such a question please do point me to his thread.
 
okay with my approach i got that that the probability is cos^2(2wT), is correct or not, i don't know, do you?
 
looks ok.
 
Well I think I miss a factor of 0.25, there.
 
my bad, I got through my calculuations and i don't think there's missing a factor.
 
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