How to Find the Time Evolution of a Polarized Cavity Mode in Quantum Mechanics?

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SUMMARY

The discussion revolves around finding the time evolution of a polarized cavity mode in quantum mechanics, specifically using the Schrödinger picture. The initial state is given as |ψ(0)> = (1/√2)(|n> + |n+1>), and the task is to derive |ψ(t)> for t > 0, evaluate the expectation of the electric field operator Ex, and calculate the uncertainty <ΔEx²>. The participant expresses difficulty with advanced quantum mechanics concepts, particularly in merging the Hamiltonian into the state and understanding the notation related to quantum harmonic oscillators (QHO).

PREREQUISITES
  • Understanding of quantum mechanics fundamentals, particularly quantum harmonic oscillators (QHO).
  • Familiarity with the Schrödinger picture and its application in quantum mechanics.
  • Knowledge of Hamiltonian operators and their role in quantum state evolution.
  • Basic proficiency in quantum notation and operators, including creation and annihilation operators.
NEXT STEPS
  • Study the derivation of time evolution in the Schrödinger picture using Hamiltonians.
  • Learn about expectation values and uncertainties in quantum mechanics, focusing on electric field operators.
  • Explore the mathematical framework of quantum harmonic oscillators, including state representations and transitions.
  • Practice problems involving the application of the Heisenberg and Schrödinger pictures in quantum mechanics.
USEFUL FOR

Students and researchers in quantum mechanics, particularly those struggling with advanced topics in cavity quantum electrodynamics and the mathematical formalism of quantum states.

danjferg
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Homework Statement


Suppose that a particular x-polarized cavity mode is described, at time t = 0, by the state

|ψ(0)> = (1/√2)(|n> + |n+1>)

Find |ψ(t)> for t > 0. This is best done in the Schrödinger picture. Evaluate the expectation of the electric field operator Ex and the uncertainty <ΔEx2>, both as a function of time. Plot your result for n = 1.​

I'm brand new to QM, and took this class after talking to the professor before the semester started. He assured me based on my past courses that I should be able to handle this class. I breezed through the first homework, but now we're doing advanced stuff using material that I have never seen before. Drop deadline passed after 1st homework so I'm stuck. I've got $5000 on the line and I really need help learning this stuff! I really need some hand-holding for these first few problems so I can learn the math and notation. My understanding of QHO is shaky at best, so this new section is really killing me.


Homework Equations



[itex]H = \hbar \sum_{j}\omega_{j}\left(\hat{a}_{j}^{\dagger}\hat{a}_{j}+\frac{1}{2}\right)[/itex]
[itex]\left[\hat{a}_{i},\hat{a}_{j}^{\dagger}\right]=\delta_{ij}[/itex]
[itex]\left[\hat{a}_{i},\hat{a}_{i}\right]=\left[\hat{a}_{i}^{\dagger},\hat{a}_{i}^{\dagger}\right]=0[/itex]

The Attempt at a Solution


I don't even know where to start. Usually I solve using the Heisenberg picture, and there I get

[itex]\left|\psi,t\right\rangle=exp\left(\frac{-iHt}{\hbar}\right)\left|\psi\right\rangle[/itex]

but I'm unclear on how to merge the Hamiltonian into the state, or exactly what the state represents. I'm looking for guidance on how to approach these problems. What, notationally, do N and N+1 represent? How do I properly set it up? I can give more details if necessary, but that is all I know to be pertinent right now.


From the Schrödinger picture I'd start with

[itex]\left|\psi\left(t\right)\right\rangle=\sum_{j}\sum_{n}c_{jn}\left|j,n\right\rangle e^{-i\left(n_{j}+1/2\right)\omega_{j}t}[/itex]

and set t=0. but how do the summations resolve (disappear from the equation)?
 
Physics news on Phys.org
What is the expectation of the electric field operator E_{x} and the uncertainty ΔE_{x}^{2}? I'm really confused on how to properly set up this problem.
 

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