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Optics Communications

Observation of the two-photon resonant parametric four-wave mixing in the NO C2Π (ν = 0) state

Juntaro Ishii, Yoshihiro Ogi, Yoshihito Tanaka, Koichi Tsukiyama∥

Published Dec 1, 1996• 16 citations
Publisher
DOI
10.1016/0030-4018(96)00365-3

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Excitons bound to neutral donors in direct gap semiconductors are known to have remarkably large oscillator strengths (f ≠ 75). This leads to extremely fast radiative lifetime (τ ≠ 50 ps). We report here the observation of large resonant degenerate four-wave mixing signals near the l2 bound exciton in high purity (~1015/cc) CdS platelets. All the incident beams propagate in the forward direction. An electrooptically modulated cw dye laser operating single mode at 487 nm is used as the optical source. Optical pulses of 2 μs in duration are produced at a repetition rate of 10 kHz. The two incident beams responsible for generating the grating in the sample are mechanically modulated at frequencies ν1 = 1527 Hz and ν2 = 1349 Hz. Phase sensitive detection is used to detect the four-wave mixing signals at ν1 + ν2. Scattering efficiently larger than 1% for peak input power levels of ~5 mW in each beam is observed. The beam diameter on the sample is ~40 μm. Resonance enhancement of the four-wave mixing signal is observed as the laser is scanned across the bound exciton resonance. An anomalously large broadening of the four-photon signal is observed as the incident intensity is increased. The possible role of light trapping is discussed.

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Parametric four-wave mixing processes in sodium vapor

Yaakov Shevy, M. Rosenbluh

Two types of parametric four-wave mixing are observed when a single intense laser beam propagates through Na vapor near the D(1) and D(2) resonance lines. The first is related to three-photon scattering, while the second results from the coherent parametric interaction of the laser with excited-state Raman scattering. Identification of the two processes was greatly facilitated by the use of an optical multichannel detector system to observe the total emission spectrum for each individual laser pulse. The experimental conditions that determine whether stimulated emission or one or both of the four-wave mixing processes dominates the emission spectrum are described.

Optics Letters•Apr 1, 1987•14 citations
Experimental investigations of two-photon enhanced stimulated hyper-Raman and parametric four-wave-mixing emissions are described for tuning unfocused laser beams near two-photon resonance with 3D and 4D states in sodium vapor. Over wide ranges of vapor pressures, path lengths, and laser power densities, the gains for stimulated hyper-Raman (SHR) scattering and for parametric four-wave mixing (PFWM) can become very greatly reduced from values expected from simple considerations. The suppression of gain can arise from interferences produced at two-photon and three-photon resonances, and from ac Stark shifts produced by internally generated near-resonant fields. Quantitative comparisons are made between observed and theoretically predicted values for SHR and PFWM production. Of 12 predicted consequences of the interferences and Stark shifting on the nonlinear behavior, ten are demonstrated through the experiments.
Excitons bound to neutral donors in direct gap semiconductors are known to have remarkably large oscillator strengths (f ≠ 75). This leads to extremely fast radiative lifetime (τ ≠ 50 ps). We report here the observation of large resonant degenerate four-wave mixing signals near the l2 bound exciton in high purity (~1015/cc) CdS platelets. All the incident beams propagate in the forward direction. An electrooptically modulated cw dye laser operating single mode at 487 nm is used as the optical source. Optical pulses of 2 μs in duration are produced at a repetition rate of 10 kHz. The two incident beams responsible for generating the grating in the sample are mechanically modulated at frequencies ν1 = 1527 Hz and ν2 = 1349 Hz. Phase sensitive detection is used to detect the four-wave mixing signals at ν1 + ν2. Scattering efficiently larger than 1% for peak input power levels of ~5 mW in each beam is observed. The beam diameter on the sample is ~40 μm. Resonance enhancement of the four-wave mixing signal is observed as the laser is scanned across the bound exciton resonance. An anomalously large broadening of the four-photon signal is observed as the incident intensity is increased. The possible role of light trapping is discussed.
Two types of parametric four-wave mixing are observed when a single intense laser beam propagates through Na vapor near the D(1) and D(2) resonance lines. The first is related to three-photon scattering, while the second results from the coherent parametric interaction of the laser with excited-state Raman scattering. Identification of the two processes was greatly facilitated by the use of an optical multichannel detector system to observe the total emission spectrum for each individual laser pulse. The experimental conditions that determine whether stimulated emission or one or both of the four-wave mixing processes dominates the emission spectrum are described.