TY - JOUR
T1 - Quantum beating in Rb at 18.3 THz (608 cm-1) detected by parametric six-wave mixing and sum-frequency generation in LiIO3
AU - Zhu, C. J.
AU - Xiao, Y.
AU - Senin, A. A.
AU - Gao, J.
AU - Eden, J. G.
AU - Varzhapetyan, T. S.
AU - Sarkisyan, D. H.
PY - 2007/5/8
Y1 - 2007/5/8
N2 - Axially phase-matched parametric six-wave mixing (PSWM) has been observed in Rb vapor by two-photon excitation of the atom (5s→→7s,5d) with ∼150 fs pulses, centered at λ∼769 nm and generated by a Ti: Al2 O3 laser system. For a peak laser pulse intensity of 30 GW cm-2, PSWM is observed for Rb number densities ([Rb])>2.5× 1015 cm-3 whereas, for [Rb]=2.2× 1016 cm-3, the PSWM process is detectable for pump intensities above ∼3 GW cm-2. Upconversion of the 1.367 μm and 1.323 μm signal waves into the visible (λ∼494 nm) has been accomplished by sum frequency generation in LiIO3, and quantum beating in Rb at 18.3 THz (∼608 cm-1) has been observed by monitoring the upconverted signal wave intensity produced in pump-probe experiments. These results broaden the scope of the wave packet detection scheme reported by Tran [Opt. Lett. 23, 70 (1998)] in that a variety of coherent nonlinear optical processes (χ(3), χ(5),...) appear to be suitable for observing the amplitude and phase of atomic (or molecular) wave packets.
AB - Axially phase-matched parametric six-wave mixing (PSWM) has been observed in Rb vapor by two-photon excitation of the atom (5s→→7s,5d) with ∼150 fs pulses, centered at λ∼769 nm and generated by a Ti: Al2 O3 laser system. For a peak laser pulse intensity of 30 GW cm-2, PSWM is observed for Rb number densities ([Rb])>2.5× 1015 cm-3 whereas, for [Rb]=2.2× 1016 cm-3, the PSWM process is detectable for pump intensities above ∼3 GW cm-2. Upconversion of the 1.367 μm and 1.323 μm signal waves into the visible (λ∼494 nm) has been accomplished by sum frequency generation in LiIO3, and quantum beating in Rb at 18.3 THz (∼608 cm-1) has been observed by monitoring the upconverted signal wave intensity produced in pump-probe experiments. These results broaden the scope of the wave packet detection scheme reported by Tran [Opt. Lett. 23, 70 (1998)] in that a variety of coherent nonlinear optical processes (χ(3), χ(5),...) appear to be suitable for observing the amplitude and phase of atomic (or molecular) wave packets.
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U2 - 10.1103/PhysRevA.75.053405
DO - 10.1103/PhysRevA.75.053405
M3 - Article
AN - SCOPUS:34347348109
SN - 1050-2947
VL - 75
JO - Physical Review A - Atomic, Molecular, and Optical Physics
JF - Physical Review A - Atomic, Molecular, and Optical Physics
IS - 5
M1 - 053405
ER -