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Quantum Electronics and Laser Science Conference

Pulse breakup in the extreme sharp-line limit

M. Matusovsky, Boris Vaynberg, M. Rosenbluh

Published Jun 7, 1996• 0 citations
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Abstract

Summary form only given. We present autocorrelation and pulse intensity data and calculations for off-resonant excitation. We observe significant pulse breakup for detunings as large as 8 nm on either side of the Cs resonance. Interestingly, the oscillation period of the broken up pulse is independent of the detuning. This is because the extremely wide laser bandwidth leaves the spectral intensity of the laser at line center nearly constant even at 8 nm detuning.

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Oscillatory emission from the Cu-vapor laser

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Our experimental studies of the optical emission from the Cu-vapor laser indicate a breakup of laser pulse into oscillatory structures in certain conditions. We believe this phenomenon is similar to the optical ringing reported earlier.1 We attribute this breakup of the pulse to cooperative effects involved in emission from the Cu-vapor laser.2 This effect is further enhanced by propagation through the system. We earlier explained the high gain of Cu-vapor due to radiation trapping and Rabi oscillation between the 2P and 2S states.3 This analysis further shows that a large percentage of Cu atoms in the lasing medium are in the excited state (2P) most of the time. Therefore, there is a very low probability for total depletion of this level. This implies that the phenomena like gain switching and relaxation oscillation may not play a significant role in the breakup of the laser pulse. The oscillatory structures for both the 510.6-nm and 578.2-nm lines were strongly dependent on the changes in operating temperature. We observed the breakup of the pulse mainly around the temperature of 1600°C.

Annual Meeting Optical Society of America•Jan 1, 1985•0 citations
Summary form only given. We present autocorrelation and pulse intensity data and calculations for off-resonant excitation. We observe significant pulse breakup for detunings as large as 8 nm on either side of the Cs resonance. Interestingly, the oscillation period of the broken up pulse is independent of the detuning. This is because the extremely wide laser bandwidth leaves the spectral intensity of the laser at line center nearly constant even at 8 nm detuning.
We observe the propagation and the reshaping of low-intensity (zero area) 60-fs pulses through high-density atomic Cs vapor. The breakup of the pulses is measured both for resonant excitation of the Cs atoms and for laser detunings such that the atomic resonance frequency is in the wings of the pulse spectrum. The theory of 0π pulse propagation in the extreme sharp-line limit is extended to include both resonant and off-resonant excitation. Good agreement is demonstrated between the observations and the theoretical predictions.
We observe the propagation and the reshaping of low intensity (zero area) 60 fs pulses through high density atomic Cs vapor. The breakup of the pulses is measured for both resonant excitation of the Cs atoms and for laser detunings such that the atomic resonance frequency is in the wings of the pulse spectrum. The theory of 0π pulse propagation, in the extreme sharp-line limit, is extended to include both resonant and off resonant excitation. Good agreement is demonstrated between the observations and the theoretical predictions.
Self-induced transparency (SIT) has been observed under the conditions of sharp-line absorption, i.e., with an inhomogeneous absorption width only one-fourth the spectral width of the pulse. A 5-nsec pulse from a 202Hg^{202}\mathrm{Hg}202Hg ii laser intersected perpendicularly an atomic beam of natural rubidium. The beam slits reduced the Doppler absorption width to about 30 MHz. A particular resolved MI{M}_{\mathrm{I}}MI​ transition of 85Rb^{85}\mathrm{Rb}85Rb was scanned into coincidence with the laser pulse by a 75-KOe magnetic field. With peak absorption depths of 3-6, nonlinear transmission, pulse delays, pulse breakup, and peak amplification were seen and found to be in excellent agreement with sharp-line computer solutions of the Maxwell-Bloch equations. The experimental realization of the sharp-line SIT is of interest because analytical formulas for pulse evolutions are more plentiful and because sharp-line SIT might permit compression of picosecond pulses.
Our experimental studies of the optical emission from the Cu-vapor laser indicate a breakup of laser pulse into oscillatory structures in certain conditions. We believe this phenomenon is similar to the optical ringing reported earlier.1 We attribute this breakup of the pulse to cooperative effects involved in emission from the Cu-vapor laser.2 This effect is further enhanced by propagation through the system. We earlier explained the high gain of Cu-vapor due to radiation trapping and Rabi oscillation between the 2P and 2S states.3 This analysis further shows that a large percentage of Cu atoms in the lasing medium are in the excited state (2P) most of the time. Therefore, there is a very low probability for total depletion of this level. This implies that the phenomena like gain switching and relaxation oscillation may not play a significant role in the breakup of the laser pulse. The oscillatory structures for both the 510.6-nm and 578.2-nm lines were strongly dependent on the changes in operating temperature. We observed the breakup of the pulse mainly around the temperature of 1600°C.