Calculating Probability of Energy Measurement in Quantum Systems

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Homework Statement



Quantum system in state |\psi\rangle. Energy of state measured at time t: Calculate probability that measurement will be E_{1}.

Homework Equations



|\psi\rangle=|1\rangle+i|2\rangle

|1\rangle is normalised stationary state with energy E_{1}. Similarly with 2.

The Attempt at a Solution



I have the time-dep Schrodinger equation for \psi as:

i \hbar \frac{\partial}{\partial t}|\psi \rangle = \hat{H}|\psi\rangle=E_{\psi}|\psi\rangle

.. but that's it.

I really don't know where to start with this :frown:
 
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First of all: To calculate probabilities you always need to normalize the states. While |1> and |2> are normalized by assumptions, what about |\psi>?
 
For normalisation of |\psi\rangle I calculated:

| |\psi\rangle |^{2}=\left(|1\rangle+i|2\rangle\right)\left(|1\rangle-i|2\rangle\right)=|1\rangle^{2}+|2\rangle^{2}
 
But what will be the normalized psi?
 
|\psi\rangle=E_{1}^{2}+E_{2}^{2} ?
 
I've still not understood this :frown:
 
You wrote:
1)
<br /> | |\psi\rangle |^{2}=\left(|1\rangle+i|2\rangle\right)\left(|1\rangle-i|2\rangle\right)=|1\rangle^{2}+|2\rangle^{2}<br />But before that:

2) |1> is normalised stationary state with ... Similarly with 2.

What can you do with 1) knowing 2)?
 
that..

| |\psi\rangle |^{2}=E_{1}^{2}+E_{2}^{2}

?
 
.. so

P(E_{1})=\frac{E_{1}^{2}}{E_{1}^{2}+E_{2}^{2}}

? or something like that
 
  • #10
So you did not read about normalization of states. And you should! That's bad!

Which is your basic textbook?
 
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