1993
DOI: 10.1007/bf01436762
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Observation of collision-induced amplified emission in Na-noble gas system

Abstract: Abstract.A stimulated resonance emission and stimulated Raman scattering signals have been generated in an atomic sodium and rare gas mixture by a laser tuned to the 32 Sin-32 P3/2 transition. The intensity dependence of these effects on the buffer gas pressures is obtained in the experiment. We demonstrate good qualitative agreement between experimental observations and a simple theoretical model. A new method using stimulated emission is applied to measure the cross section for the J mixing of 3P states of s… Show more

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Cited by 11 publications
(3 citation statements)
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“…The collisional energy transfer mechanism is employed in CO 2 lasers, for example, where helium atoms are introduced, to increase the efficiency of the CO 2 lasing process. In atomic alkali metal vapors, the emission is amplified through mixing with helium [45][46][47] to utilize collisional energy transfer for increasing the lasing output.…”
Section: Discussionmentioning
confidence: 99%
“…The collisional energy transfer mechanism is employed in CO 2 lasers, for example, where helium atoms are introduced, to increase the efficiency of the CO 2 lasing process. In atomic alkali metal vapors, the emission is amplified through mixing with helium [45][46][47] to utilize collisional energy transfer for increasing the lasing output.…”
Section: Discussionmentioning
confidence: 99%
“…The system is pumped on the D 2 line at 780 nm and lases on the D 1 line at 795 nm. 5 It has been long recognized in the scientific literature [1,2] that population inversions can be produced on the D 1 transition of alkali atoms, by resonantly pumping the D 2 transition with a dye laser, and ASE has been observed. However, up until now the extension of this work to an efficient optically excited atomic alkali vapor laser has been hampered by two issues:…”
Section: Introductionmentioning
confidence: 99%
“…[5][6][7][8][9][10][11][12][13]. Numerous theoretical and experimental studies of energy transfer, energy levels mixing, and a three-level lasing in alkalis were performed during that time, [14][15][16][17][18][19][20][21][22][23][24][25][26][27] but an absence of powerful enough narrowband tunable pump laser sources did not allow efficient lasing in alkali vapors until the beginning of the new millennium. The first really efficient lasing in pulsed and continuous wave (CW) operation in Rb and Cs vapors was observed in 2003 to 2005, 28,29 using a Ti:sapphire laser for optical pumping.…”
Section: Introductionmentioning
confidence: 99%