Chapter 15: Strong Field Excitation
Calculation of the evolution of the population in a 3-level A system using the STIRAP scheme (bare state representation).
level |2>, and |2> to |3> but |1> not- directly to |3> In a rotating frame, and making the RWA the Schrödingcr equation can be written:
with A sufficient condition for the population in level |2> to remain approximately 0 is that In physical terms, the time rate of change of involves two contributions, that from level |1> and that from level |3>. If these two contributions are equal and opposite, the population in level |2> will remain constant. At early times, when is large and is small, must be small and must be large in order for the contributions to cancel; at late times the situation is reversed. This is a simple but unconventional interpretation of the counterintuitive ordering of the pulses in the STIRAP scheme.
with A sufficient condition for the population in level |2> to remain approximately 0 is that In physical terms, the time rate of change of involves two contributions, that from level |1> and that from level |3>. If these two contributions are equal and opposite, the population in level |2> will remain constant. At early times, when is large and is small, must be small and must be large in order for the contributions to cancel; at late times the situation is reversed. This is a simple but unconventional interpretation of the counterintuitive ordering of the pulses in the STIRAP scheme.