Quantum Mechanics: Harmonic Oscillator

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The discussion centers on a quantum harmonic oscillator where a particle can be in a superposition of the ground state and first excited state, represented as |ψ⟩ = c₁|0⟩ + c₂|1⟩, with equal probabilities for measuring energies of ħω/2 and 3ħω/2. The average momentum ⟨pₓ⟩ at time t=0 is calculated to be √(mωħ/2), and the calculation involves the properties of the raising and lowering operators. Participants seek clarification on why ⟨0|a|1⟩ and ⟨1|a†|0⟩ equal one, emphasizing the importance of the operators in determining state transitions. The conversation highlights the need for understanding the specifics of quantum states and their energy levels in the context of harmonic oscillators.
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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