Adiabatic theorem for a 3 level system

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SUMMARY

The discussion centers on the application of the adiabatic theorem to a three-level quantum system characterized by energy levels E1, E2, and E3. The user explores the conditions under which the adiabatic approximation can be applied, specifically when the frequency of the external perturbation (ωP) is much greater than the energy splitting between levels (ω12) but much less than the splitting between the higher levels (ω23). The user proposes that under these conditions, the coupling term f12(t) can be neglected, allowing for a simplified Hamiltonian representation. However, they also acknowledge the potential for missing transitions from level 1 to level 3 via level 2, indicating a trade-off in approximation accuracy.

PREREQUISITES
  • Understanding of quantum mechanics and the Schrödinger equation (SE).
  • Familiarity with the adiabatic theorem and its implications in quantum systems.
  • Knowledge of Hamiltonian mechanics and matrix representations of quantum states.
  • Concept of energy level splitting and perturbation theory in quantum systems.
NEXT STEPS
  • Study the adiabatic theorem in detail, focusing on its mathematical formulation and applications.
  • Learn about perturbation theory in quantum mechanics, particularly in multi-level systems.
  • Investigate the implications of neglecting certain coupling terms in Hamiltonians.
  • Explore numerical methods for solving the Schrödinger equation in complex quantum systems.
USEFUL FOR

Quantum physicists, researchers in quantum mechanics, and students studying multi-level quantum systems will benefit from this discussion, particularly those interested in the adiabatic approximation and its applications in quantum transitions.

Malamala
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Hello! If I have a 2 level system, with the energy splitting between the 2 levels ##\omega_{12}## and an external perturbation characterized by a frequency ##\omega_P##, if ##\omega_{12}>>\omega_P## I can use the adiabatic approximation, and assume that the initial state of the system changes slowly in time while for ##\omega_{12}<<\omega_P## I can assume that the perturbation doesn't have any effect on the system (it averages out over the relevant time scales). I was wondering if I have a 3 level system with ##E_1<E_2<E_3## such that ##\omega_{12}<<\omega_P<<\omega_{23}##. In general, the Hamiltonian of the system would look like this:

$$
\begin{pmatrix}
E_1 & f_{12}(t) & f_{13}(t) \\
f_{12}^*(t) & E_2 & f_{23}(t) \\
f_{13}^*(t) & f_{23}^*(t) & E_3
\end{pmatrix}
$$

But using the intuition from the 2 level system case, can I ignore ##f_{12}(t)##, as the system of these 2 levels (1 and 2) moves on time scales much slower than ##\omega_P##, and assume that ##f_{23}(t)## and ##f_{13}(t)## move very slow and thus use the adiabatic approximation? In practice I would basically have:

$$
\begin{pmatrix}
E_1 & 0 & f_{13}(t) \\
0 & E_2 & f_{23}(t) \\
f_{13}^*(t) & f_{23}^*(t) & E_3
\end{pmatrix}
$$

Or in this case I would need to fully solve the SE, without being able to make any approximations? Thank you!
 
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Seems like a reasonable approach to me. This might miss some processes transiting from 1 to 3 via 2, but this is all about making approximations.
 

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