When is the Interaction representation used and why?

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SUMMARY

The Interaction representation, also known as the Interaction picture, is a crucial tool in quantum mechanics that facilitates the application of time-dependent perturbation methods. It serves as a bridge between the Schrödinger and Heisenberg pictures, allowing for convenient transitions via unitary transformations. This representation is particularly beneficial when analyzing systems like the driven Jaynes-Cummings Hamiltonian at resonance, where it simplifies the problem by effectively eliminating time dependence and reducing the complexity of the Hamiltonian. While not strictly necessary, the Interaction picture enhances problem-solving efficiency in quantum mechanics.

PREREQUISITES
  • Understanding of quantum mechanics principles, specifically Hamiltonians
  • Familiarity with the Schrödinger and Heisenberg pictures
  • Knowledge of time-dependent perturbation theory
  • Basic grasp of unitary transformations in quantum systems
NEXT STEPS
  • Study time-dependent perturbation theory in quantum mechanics
  • Learn about the Jaynes-Cummings model and its applications
  • Explore unitary transformations and their role in quantum mechanics
  • Investigate the differences between the Schrödinger, Heisenberg, and Interaction pictures
USEFUL FOR

Quantum physicists, students of quantum mechanics, and researchers working on time-dependent systems will benefit from this discussion, particularly those interested in simplifying complex Hamiltonian problems.

DonnerJack
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Hi,

Can someone explain to me why do we actually need the Interaction/Intermediate representation?
In my past, each course in QM touched it only for a few minutes and then it got... forgotten.

Can someone please give me an example as to how (and when) it is used (and a good reason why)?

Thanks!
 
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the interaction picture is useful because it's decomposition of the hamiltonian allows for time-dependent perturbation methods
 
We don't really "need" the interaction picture, but it is very convenient sometimes.
The interaction picture is a representation which is somewhere in-between the Schrödinger and the Heisenberg picture. Note, however, that you can easily move between all of these representations using unitary transformations.

I think the word "picture" is somewhat missleading. Today there is no "philosophical" reason why you choose one over the other, you use whichever one s the most convenient for the problem you are trying to do. Moving between pictures is therefore somewhat akin to e.g. moving between coordinate-systems in classical mechanics.

A good example would be a driven Jaynes-Cummings Hamiltonian on resonance (being driven at some frequency [tex]$\omega_l=\omega_0=\omega_r$, where $\omega_0, \omega_r$[/tex] are the splitting of the 2-level system and the resonance frequency of the resonator, respectively).
Moving to the interaction picture here essentially means that you are solving your problem in a 'rotating coordinate system' which simplifies the problem A LOT since all but two terms become zero and the time dependence dissapears.
 

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