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Stimulated raman adiabatic passage : ウィキペディア英語版 | Stimulated raman adiabatic passage
The Stimulated Raman adiabatic passage (STIRAP) process permits transfer of a population between two applicable quantum states via at least two coherent electromagnetic (light) pulses. These light pulses drive the transitions of the three level Ʌ atom or multilevel system.〔Unanyan, R., M. Fleischhauer, B. W. Shore, and K. Bergmann. "Robust creation and phase-sensitive probing of superposition states via stimulated Raman adiabatic passage (STIRAP) with degenerate dark states." Optics communications 155, no. 1 (1998): 144-154.〕 The process is a form of state-to-state coherent control. ==Population transfer in three level Ʌ atom== Consider the description of three level Ʌ atom having ground state and (for simplicity consider the energy of both ground states are same) and excited state respectively. Suppose in the beginning the total population is in the ground state . Here the logic for transformation of the population from ground state to is that initially the unpopulated states and couple, afterward superposition of state and couple to the state . Thereby a state is formed that permits the transformation of the population into state without populating the excited state . This process of transforming the population without populating the excited state is called the stimulated Raman adiabatic passage.
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