How Does the Rotating Wave Approximation Simplify the Density Matrix Evolution?

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SUMMARY

The discussion focuses on the Rotating Wave Approximation (RWA) and its application to the evolution of the density matrix in a two-level quantum system. The original frame's time derivative of the density matrix's first diagonal element is expressed as \(\frac{d\rho_{11}}{dt} = i e^{i\omega_r t} K \rho_{21} - i e^{-i\omega_r t} K^* \rho_{12}^*\). In the rotating frame of frequency \(\omega_r\), this simplifies to \(\frac{d\rho_{11}}{dt} = i K \rho_{21} - i K^* \rho_{12}^*\). The discussion highlights the importance of maintaining the diagonal elements unchanged during the transformation, emphasizing that the RWA is a unitary transformation rather than merely removing a global phase.

PREREQUISITES
  • Understanding of quantum mechanics, specifically two-level systems
  • Familiarity with density matrix formalism
  • Knowledge of unitary transformations in quantum mechanics
  • Basic grasp of the Rotating Wave Approximation (RWA)
NEXT STEPS
  • Study the mathematical derivation of the Rotating Wave Approximation (RWA)
  • Explore the implications of unitary transformations on quantum states
  • Learn about the role of density matrices in quantum mechanics
  • Investigate applications of the RWA in quantum optics and quantum information
USEFUL FOR

Quantum physicists, researchers in quantum mechanics, and students studying two-level systems will benefit from this discussion, particularly those interested in the Rotating Wave Approximation and density matrix evolution.

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In a text, it introduces an rotating frame and applies it on evolution of density matrix of two-level system. In the original frame, the first diagonal element of the time-derivitative of density matrix gives

[tex]\frac{d\rho_{11}}{dt} = i e^{i\omega_r t} K \rho_{21} - i e^{-i\omega_r t} K^* <br /> \rho_{12}^*[/tex]

In rotating frame of freq [tex]\omega_r[/tex], it gives

[tex]\frac{d\rho_{11}}{dt} = i K \rho_{21} - i K^* \rho_{12}^*[/tex]

I don't really understand how to get above result. In my opinion, I will factor out [tex]e^{i\omega_r t}[/tex] such that

[tex]\frac{d\rho_{11}}{dt} = i e^{i\omega_r t}\left[ K \rho_{21} - e^{-i2\omega_r t} K^* \rho_{12}^*\right][/tex]

and now in the rotating frame, it gives
[tex]\frac{d\rho_{11}}{dt} = i \left[ K \rho_{21} - e^{-i2\omega_r t} K^* \rho_{12}^*\right][/tex]

But there are some extra term [tex]e^{-i2\omega_r t}[/tex] left, I know this is not the correct result but how to get the correct one?

By the way, in the text, seems like it only consider the off-diagonal density matrix element is of the form [tex]e^{i\omega_r t}\rho_{12}[/tex] or [tex]e^{-i\omega_r t}\rho_{21}[/tex] but let all diagonal term unchanged (i.e. no [tex]e^{\pmi\omega_r t}[/tex]), why is that?
 
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The first step in the RWA is to go to the rotating reference frame, which is a unitary transform. This is not the same a removing a global complex phase.

https://arxiv.org/abs/1301.3585
 

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