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Controlling atomic states by optical pulses

K. Igeta, Bernd Hüttner, Nobuyuki Imoto

Published Aug 24, 2005• 0 citations
Publisher
DOI
10.1109/cleopr.1995.527049

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We report a study of the optical dipole force on a beam of neutral three-level, $\ensuremath{\Lambda}$-like atomic system induced by a femtosecond super-Gaussian pulse. We show that maximum coherence between the ground state $|1\ensuremath{\rangle}$ and the excited state $|2\ensuremath{\rangle}$ could be achieved using a train of femtosecond pulses. In addition, it is possible to control the trajectory of the atoms in an atomic beam by using the same scheme. The robustness of the scheme against the variation of the pulse parameters is also investigated.
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We develop a pulse-driven jump protocol to achieve all-optical Raman control of ultracold atomic hyperfine states. By establishing general conditions for adiabatic evolution between quantum states in parameter space, we derive the essential pulse area and phase conditions necessary for quantum state transfer in a resonant single-ΛΛΛ three-level system. We extend this approach to a double-ΛΛΛ four-level system by incorporating a neighboring intermediate state, which leads to a single-photon detuned ΛΛΛ three-level system. Through numerical simulations of the ultracold 87^{87}87Rb atomic system, we demonstrate that high-fidelity and robust control of quantum state transfer can be achieved in the single-ΛΛΛ three-level system using stimulated Raman adiabatic passage (STIRAP) and the pulsed jump protocol. Furthermore, we show that the destructive quantum interference effects between resonant and detuned Raman pathways in the double-ΛΛΛ four-level system can be mitigated by optimizing the pulse area and two-photon detuning parameters within the pulsed jump protocol. This work presents a promising approach for achieving all-optical Raman control of quantum state transfer in ultracold atomic hyperfine states.