How do you find the probabilities for an anharmonic quantum oscillator state?

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SUMMARY

The discussion centers on calculating the probabilities for an anharmonic quantum oscillator state, specifically starting from the state ##| \Psi (t) \rangle = | 1 \rangle## at ##t=0##. The perturbation is defined as ##V(x)=\alpha x^3 = \alpha (\frac{\hbar}{2m\omega})^{3/2} (a+a^{\dagger})^3 = \gamma (a^3+3Na+3Na^{\dagger} + 3a + (a^{\dagger})^3)##. The corrected state is expressed as ##|\Psi \rangle = |1 \rangle + c_0|0 \rangle + c_2|2 \rangle + c_4|4\rangle##, where ##c_k = \langle k| V(x) | 1 \rangle##. The probabilities for the oscillator in states ##|n \rangle## are derived as ##P_k = |c_k|^2/\langle \Psi |\Psi \rangle##, addressing normalization issues in the calculations.

PREREQUISITES
  • Understanding of quantum mechanics, specifically quantum harmonic oscillators
  • Familiarity with perturbation theory in quantum mechanics
  • Knowledge of bra-ket notation and inner products in quantum states
  • Basic grasp of operators in quantum mechanics, particularly creation and annihilation operators
NEXT STEPS
  • Study perturbation theory in quantum mechanics, focusing on anharmonic oscillators
  • Learn about normalization conditions for quantum states and their implications
  • Explore the mathematical derivation of the coefficients ##c_k = \langle k| V(x) | 1 \rangle##
  • Investigate the properties of creation and annihilation operators in quantum mechanics
USEFUL FOR

Quantum physicists, students studying quantum mechanics, and researchers working on quantum harmonic oscillators and perturbation theory will benefit from this discussion.

damarkk
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Homework Statement
Find the probability for all possible unperturbed states ##| n\rangle## for an harmonic oscillator with perturbation ##V(x)=\alpha x^3##
Relevant Equations
##x##, ##p##.
I have one tremendous doubt about it.


On ##t=0## the state of the oscillator is ##| \Psi (t) \rangle = | 1 \rangle ##. The perturbation is ##V(x)=\alpha x^3 = \alpha (\frac{\hbar}{2m\omega})^{3/2} (a+a^{\dagger})^3 = \gamma (a^3+3Na+3Na^{\dagger} + 3a + (a^{\dagger})^3)##.

The only possible other states are ##|0 \rangle##, ##| 2\rangle##, ##|4\rangle##. The state corrected on the first order is:

##|\Psi \rangle = |1 \rangle + c_0|0 \rangle + c_2|2 \rangle + c_4|4\rangle##

where ##c_k = \langle k| V(x) | 1 \rangle ##.


What are the probability to find the oscillator in a generic state ##|n \rangle##?


My answer is ##P_k = |c_k|^2##, but for k=1 we have ##P_1 = 1##. This is not possible I think. On the other hand, I suppose that ##P_1 = 1-P_0 - P_2- P_4 = 1-|c_0|^2-|c_2|^2-|c_4|^2##, but how can I show this? The coefficient of ##| 1\rangle## is 1. This is my question.
 
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damarkk said:
Homework Statement: Find the probability for all possible unperturbed states ##| n\rangle## for an harmonic oscillator with perturbation ##V(x)=\alpha x^3##
Relevant Equations: ##x##, ##p##.

On ##t=0## the state of the oscillator is ##| \Psi (t) \rangle = | 1 \rangle ##.
How do you know the state is ##|1\rangle## at ##t = 0##? This was not given in the homework statement as given. Always provide the full homework statement.

I don't understand "##x##, ##p##" for your Relevant Equations.
damarkk said:
The perturbation is ##V(x)=\alpha x^3 = \alpha (\frac{\hbar}{2m\omega})^{3/2} (a+a^{\dagger})^3 = \gamma (a^3+3Na+3Na^{\dagger} + 3a + (a^{\dagger})^3)##.

The only possible other states are ##|0 \rangle##, ##| 2\rangle##, ##|4\rangle##. The state corrected on the first order is:

##|\Psi \rangle = |1 \rangle + c_0|0 \rangle + c_2|2 \rangle + c_4|4\rangle##

where ##c_k = \langle k| V(x) | 1 \rangle ##.
Your expression for ##c_k## doesn't have the correct dimensions. Did you leave out something?

damarkk said:
What are the probability to find the oscillator in a generic state ##|n \rangle##?


My answer is ##P_k = |c_k|^2##, but for k=1 we have ##P_1 = 1##. This is not possible I think. On the other hand, I suppose that ##P_1 = 1-P_0 - P_2- P_4 = 1-|c_0|^2-|c_2|^2-|c_4|^2##, but how can I show this? The coefficient of ##| 1\rangle## is 1. This is my question.
From ##|\Psi \rangle = |1 \rangle + c_0|0 \rangle + c_2|2 \rangle + c_4|4\rangle##, you can see that ##|\Psi \rangle## is not normalized.

That's ok. The probability ##P_k## is then ##|c_k|^2/\langle \Psi |\Psi \rangle##.
 

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