How to Find Probabilities in Quantum Mechanics?

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To find probabilities in quantum mechanics, the probability of measuring a state |\psi\rangle in a state |\phi\rangle is calculated using the formula \left| \left<\phi \middle| \psi \right>\right|^2. For the given wave function with l = 1, the probabilities for the states \hbar, 0, and -\hbar can be derived from the normalized angular momentum eigenstates. The calculations yield probabilities of \frac{1}{14} for \hbar, \frac{2}{7} for 0, and \frac{9}{14} for -\hbar. Understanding how to apply these concepts is crucial for solving quantum mechanics problems effectively.
Biest
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Hi,

I have a quick homework problem because I am confused. So a wave function with l = 1 in the state:

|\psi&gt; = \frac{1}{\sqrt{14}} \[ \left( \begin{array}{ccc}<br /> 1 \\<br /> 2 \\<br /> 3i \end{array} \right)\]

and i have to find the probability to be in state \hbar, -\hbar, 0 in L_z, so i applied L_z so |\psi&gt; and got

L_z|\psi&gt; = \frac{\hbar}{\sqrt{14}} \[ \left( \begin{array}{ccc}<br /> 1 \\<br /> 0 \\<br /> -3i \end{array} \right)\]

How do i find the probabilities from that?Thanks,

Biest
 
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Always, the probability of finding a state |\psi\rangle in a state |\phi\rangle is \left| \left&lt;\phi \middle| \psi \right&gt;\right|^2.
 
But how do i take the \hbar, -\hbar 0 condition into account?
 
assuming your |\psi\rangle is in the basis of normalised angular momentum eigenstates, then your probabilities just correspond to \frac{1}{14} for \hbar, \frac{2}{7} for 0 and \frac{9}{14} for -\hbar.

so what happens is that for |\phi\rangle to return you an eigenvalue of say \hbar, we need

|\phi\rangle = \[ \left( \begin{array}{ccc} 1 \\ 0 \\ 0 \end{array} \right) \]

and taking \left| \left&lt;\phi \middle| \psi \right&gt;\right|^2, we get \frac{1}{14}.

hope it helps. QM was never my strong point. haha
 

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