Quantum Mechanics Superposition Question

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SUMMARY

The discussion centers on calculating the time-dependent wavefunction |ψ(x,t)|² for a particle in an infinite square well, given the initial wavefunction ψ(x,t=0) = (1/√2)[φ1 + φ3]. The participant correctly identifies the wavefunction as ψ(x,t) = (1/√2)[e^(-iω1t)φ1 + e^(-iω3t)φ3], where ω = π²h/(2mL²) is the angular frequency related to the energy states. The relationship between ω and the energy of state n is clarified through the equation ω_n = E_n/ħ, establishing a direct connection between the two.

PREREQUISITES
  • Understanding of quantum mechanics concepts, specifically wavefunctions and superposition.
  • Familiarity with the infinite square well model in quantum mechanics.
  • Knowledge of angular frequency and its relation to energy states.
  • Proficiency in mathematical expressions involving complex exponentials and sinusoidal functions.
NEXT STEPS
  • Study the derivation of the infinite square well wavefunctions φn = √(2/L)sin(nπx/L).
  • Learn about the time evolution of quantum states using the Schrödinger equation.
  • Explore the relationship between energy levels and angular frequency in quantum mechanics.
  • Investigate the implications of superposition in quantum systems and its measurement outcomes.
USEFUL FOR

Students and educators in quantum mechanics, particularly those focusing on wavefunctions, superposition, and the infinite square well model. This discussion is also beneficial for anyone looking to deepen their understanding of quantum state evolution.

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Homework Statement


A particle in an infinite square well has as its initial wavefunction ψ(x,t=0) = (1/√2)[φ1 + φ3].

Find |ψ(x,t)|2. Express it as a sinusoidal function of time using ω= π2*h/(2mL2).

Homework Equations


Note that φn = √(2/L)*sin(nπx/L) for a well of width L.

The Attempt at a Solution



I found something in my book which says that ψ(x,t) = Ʃbn*e-iωntφn.

Therefore, my ψ(x,t) = (1/√2)[e-iω1t)φ1 + e-iω3t)φ3].

Is that right so far?

Then, I can compute |ψ(x,t)|2, but I don't see how that is going to give me an answer in terms of ω. I have ωn though.
 
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How are ##\omega## and ##\omega_n## related to the energy of state n?
 
When you say you found something in your book that says [itex]\Psi (x,t) = \sum_n b_n\ e^{-i\ \omega _n \ t}\ \psi _n(x)[/itex], do you know what that is?
Also, do you know what [itex]\omega _n[/itex] actually is?
 
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