Chapter 15: Strong Field Excitation
Calculation of the evolution of the population in a 3-level A system using the STIRAP scheme (dressed state representation).
In the rotating frame and making the RWA the Hamiltonian can be written:
with This matrix can be diagonalized yielding the eigenvalues, and eigenvectors
Where The eigenvectors are dressed states, i.e. eigenfunctions of the instantaneous Hamiltonian in the presence of the fields. Consider the adiabatic change in field intensities such that for while for This adiabatic transformation will leave the system in the dressed state while changing its character from that of level |1> to that of level |3>. Since the dressed state contains no component of level |2>, this adiabatic change leads to complete population transfer from level |1> to level |3>, without populating level |2>. This is the basis for the remarkable Stimulated Raman Adiabatic Passage (STIRAP) scheme. Note the counterintuitive order of the pulses, i.e. precedes .
In the rotating frame and making the RWA the Hamiltonian can be written:
with This matrix can be diagonalized yielding the eigenvalues, and eigenvectors
Where The eigenvectors are dressed states, i.e. eigenfunctions of the instantaneous Hamiltonian in the presence of the fields. Consider the adiabatic change in field intensities such that for while for This adiabatic transformation will leave the system in the dressed state while changing its character from that of level |1> to that of level |3>. Since the dressed state contains no component of level |2>, this adiabatic change leads to complete population transfer from level |1> to level |3>, without populating level |2>. This is the basis for the remarkable Stimulated Raman Adiabatic Passage (STIRAP) scheme. Note the counterintuitive order of the pulses, i.e. precedes .