BREAD
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DrClaude said:You don't start the problem correctly. The ##|S_z = + \hbar/2 \rangle## state is not an eigenstate of the Hamiltonian, so after a time ##T_2##, the state of the system is not ##e^{-i E T_2 / \hbar} |S_z = + \hbar/2 \rangle##.
In the problem, megnetic field is Bx direction.DrClaude said:In which direction is the magnetic field?
Sx * BDrClaude said:So how can you rewrite ##\mathbf{S} \cdot \mathbf{B}##?
DrClaude said:You have to express the initial state in terms of the eigenstates of the Hamiltonian.
DrClaude said:Don't forget the normalization factor.
But now that the state is expressed in terms of the eigenstates of the Hamiltonian, it should be easy to calculate the time evolution.
I replied the answer that i triedDrClaude said:Why? This is a very standard problem in QM and illustrates nicely the concept of precession.
I got it, then how can i approach problem(b) i think the result of first measurement is same with (a)DrClaude said:Ok, I had replied before you posted the solution.
There is a problem, as you can clearly see that the prbability you get ranges from 0 to 2. Check again how you calculate the absolute value squared.
The probability of measuring Sz = +ħ/2 is indeed given by the same equation, replacing T2 by T1. But you already know the measurement result, so you need to figure out what you get at T2.BREAD said:I got it, then how can i approach problem(b) i think the result of first measurement is same with (a)
DrClaude said:The probability of measuring Sz = +ħ/2 is indeed given by the same equation, replacing T2 by T1. But you already know the measurement result, so you need to figure out what you get at T2.
By the way, you can simplify the result you get using explicit values for E1 and E2.