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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 |g_1\rangle and |g_2\rangle (for simplicity consider the energy of both ground states are same) and excited state |e\rangle respectively. Suppose in the beginning the total population is in the ground state |g_1\rangle . Here the logic for transformation of the population from ground state |g_1\rangle to |g_2\rangle is that initially the unpopulated states |g_2\rangle and |e\rangle couple, afterward superposition of state |g_2\rangle and |e\rangle couple to the state |g_1\rangle . Thereby a state is formed that permits the transformation of the population into state |g_2\rangle without populating the excited state |e\rangle . This process of transforming the population without populating the excited state is called the stimulated Raman adiabatic passage.

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