1989
DOI: 10.1070/qe1989v019n06abeh008116
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Quasi-cw λ = 585.3 nm stimulated emission from Ne generated by pumping an Ne–H2mixture with a low-energy electron beam

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“…A high degree of ionization followed by recombination is obtained due to the beam component of non-Maxwellian electrons with energies of 1-2 keV in the tail of the electron energy distribution function. Lasing on the NeI 585.3 nm line with a peak output power of several watts and a gain of several m −1 has been obtained [9,[13][14][15].…”
Section: Introductionmentioning
confidence: 96%
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“…A high degree of ionization followed by recombination is obtained due to the beam component of non-Maxwellian electrons with energies of 1-2 keV in the tail of the electron energy distribution function. Lasing on the NeI 585.3 nm line with a peak output power of several watts and a gain of several m −1 has been obtained [9,[13][14][15].…”
Section: Introductionmentioning
confidence: 96%
“…It is of practical interest to realize PRLs in gas discharges having a beam of high-energy primary electrons. Lasing has been obtained by using special types of discharges such as the fast transverse discharge [5,8], open discharge [9], discharges with pre-ionization [10,11] and microwave discharges [12]. Various mixtures-He-Ne-Ar (Kr), Ne-Ar, Ne-H 2 and Ne-NF 3 have been used as an active medium and lasing on eight NeI lines has been obtained.…”
Section: Introductionmentioning
confidence: 99%