2018
DOI: 10.1364/josab.35.003014
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Robust switching of superposition-states via a coherent double stimulated Raman adiabatic passage

Abstract: Coherent manipulation of quantum states is of crucial importance in accurate control of a quantum system. A fundamental goal is coherently transferring the population of a desired state with near-unit fidelity. For this propose, we theoretically demonstrate a novel coherent double-stimulated Raman adiabatic passage (STIRAP) in a three-level Λ-type system for realizing the switch of unequal initial preparations on two ground states. This operation uses single optical pulse sequence accomplishing both bright-STI… Show more

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“…by combining them with composite pulses, similarly to the design robust adiabatic pulses in two-state systems. We note that previous work [25] has also discussed exchanging the populations of two ground states in a three-level system by STIRAP but it required very careful adjustment of the single-photon detuning and pulse delay for achieving high fidelity. In contrast, our work (1) demonstrates that swapping is possible for a wide range of the single-photon detuning as long as adiabaticity is maintained, (2) it considers swapping the populations of coherent superposition states and statistical mixtures and the differences between these cases, and (3) it shows that while single STIRAP is sensitive to the dynamic phase η ± (see equation ( 12)), it can be applicable for spin refocusing by , e.g.…”
Section: Discussionmentioning
confidence: 99%
“…by combining them with composite pulses, similarly to the design robust adiabatic pulses in two-state systems. We note that previous work [25] has also discussed exchanging the populations of two ground states in a three-level system by STIRAP but it required very careful adjustment of the single-photon detuning and pulse delay for achieving high fidelity. In contrast, our work (1) demonstrates that swapping is possible for a wide range of the single-photon detuning as long as adiabaticity is maintained, (2) it considers swapping the populations of coherent superposition states and statistical mixtures and the differences between these cases, and (3) it shows that while single STIRAP is sensitive to the dynamic phase η ± (see equation ( 12)), it can be applicable for spin refocusing by , e.g.…”
Section: Discussionmentioning
confidence: 99%