Quantum Mechanics: Harmonic Oscillator

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Homework Help Overview

The discussion revolves around a quantum mechanics problem involving a one-dimensional harmonic oscillator. The original poster presents a scenario where a particle's energy measurements yield specific values with given probabilities, and they seek to understand the state of the particle and the average momentum at a later time.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants explore the nature of the state represented as a superposition of energy eigenstates and question the reasoning behind this representation. They also discuss the implications of the raising and lowering operators in relation to the energy states.

Discussion Status

Some participants have provided insights into the properties of the raising and lowering operators, while others continue to seek clarification on how the state of the particle is determined from the given energy measurements. There is an ongoing exploration of the relationships between the operators and the energy eigenstates.

Contextual Notes

Participants are examining the definitions and properties of quantum states and operators, with a focus on the implications of superposition in the context of the harmonic oscillator. There is a noted lack of consensus on the interpretation of certain mathematical expressions related to the operators.

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



None

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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