1982
DOI: 10.1016/0030-4018(82)90331-5
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Gain limitations in CO2 lasers

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Cited by 10 publications
(4 citation statements)
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“…No indications of the saturation of the temperature T 3 with increase in the pumping energy W p were noted. The high values of the gain coefficient and T 3 are attributed in [16] to the absence of the mechanism of de-excitation by electrons of the upper laser level 00 0 1 in an optical-pumping system, and these results are considered as confirmation of the earlier conclusion [5][6][7][8][9][10] that precisely the de-excitation by electrons restricted the excitation of the ν 3 mode and, consequently, also amplification in electricdischarge CO 2 lasers.…”
Section: Introductionsupporting
confidence: 69%
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“…No indications of the saturation of the temperature T 3 with increase in the pumping energy W p were noted. The high values of the gain coefficient and T 3 are attributed in [16] to the absence of the mechanism of de-excitation by electrons of the upper laser level 00 0 1 in an optical-pumping system, and these results are considered as confirmation of the earlier conclusion [5][6][7][8][9][10] that precisely the de-excitation by electrons restricted the excitation of the ν 3 mode and, consequently, also amplification in electricdischarge CO 2 lasers.…”
Section: Introductionsupporting
confidence: 69%
“…It is seen that for the same quantity of vibrational energy expressions (3) and (8) put into correspondence different values of the vibrational temperature T 3 , with formula (3) yielding a lower value of T 3 in comparison with that given by Eq. (8). The use of these data together with the measured gain coefficient leads to understated values of the vibrational temperatures T 1 and T 2 and, as a consequence, to incorrect interpretation of the physical processes proceeding in the active medium [14].…”
Section: Introductionmentioning
confidence: 99%
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