Quantum Mechanics: Harmonic Oscillator

Robben
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Homework Statement



A particle of mass m in the one-dimensional harmonic oscillator is in a state for which a measurement of the energy yields the values ##\hbar\omega/2## or ##3\hbar\omega/2## each with a probability of one-hald. The average value of the momentum ##\langle p_x\rangle## at time ##t=0## is ##\sqrt{m\omega\hbar/2}##. What is this state and what is ##\langle p_x\rangle## at time ##t##?

Homework Equations



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The Attempt at a Solution



The solution states that since ##|\psi\rangle## is the superposition of ##n=0## and ##n=1## then ##|\psi\rangle = c_1|0\rangle +c_2|1\rangle## but why is that? What information specifies the state of the particle?

It goes on by calculating $$|psi\rangle =
\frac{1}{\sqrt{2}}(|0\rangle+e^{i\phi}|1\rangle)$$ $$\langle p_x\rangle=-i\sqrt{m\omega\hbar}/2\langle\psi|(a-a^{\dagger})|\psi \rangle$$ $$=\frac{-i}{2}\sqrt{\frac{m\omega\hbar}{2}}(e^{i\phi}\langle0|a|1\rangle-e^{-i\phi}\langle1|a^{\dagger}|0\rangle)$$ but why does ##\langle0|a|1\rangle## and ##\langle1|a^{\dagger}|0\rangle## equal one?
 
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Robben said:
What information specifies the state of the particle?
The part saying that is in a superposition of two of the energy eigenstates.
Robben said:
but why does ⟨0|a|1⟩\langle0|a|1\rangle and ⟨1|a†|0⟩\langle1|a^{\dagger}|0\rangle equal one?

What are the properties of the raising and lowering operators?
 
Orodruin said:
The part saying that is in a superposition of two of the energy eigenstates.

What are the properties of the raising and lowering operators?

Oh, I see for the second part of my question. Thank you. For the first part I am still not sure how they got ##|\psi\rangle = c_1|0\rangle +c_2|1\rangle##.
 
Robben said:
is in a state for which a measurement of the energy yields the values ##\hbar\omega/2## or ##3\hbar\omega/2##
Which states have an energy of ##\hbar\omega/2## and ##3\hbar\omega/2##?
 
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