Numerical study of overpopulation density for laser oscillation in recombining hydrogen plasmas
Overpopulation densities Δ n itij , which are defined as the differences between the population densities per unit statistical weight of the upper and lower excited levels i and j, are calculated as a function of the electron density n e for various electron temperatures T e in recombining hydrogen...
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Published in | Journal of quantitative spectroscopy & radiative transfer Vol. 29; no. 6; pp. 553 - 559 |
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Main Authors | , |
Format | Journal Article |
Language | English |
Published |
Elsevier Ltd
01.06.1983
|
Online Access | Get full text |
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Summary: | Overpopulation densities Δ
n
itij
, which are defined as the differences between the population densities per unit statistical weight of the upper and lower excited levels
i and
j, are calculated as a function of the electron density
n
e
for various electron temperatures
T
e
in recombining hydrogen plasmas. Calculation have been made for line pairs with principal quantum numbers (2 ,3), (3, 4) and (4, 5). The effect of the ground-level population density
n
1 on Δ
n
ij
is calculated. In this calculation, the atom-atom collision and the self-absorption of the resonance lines are taken into account. The
n
1-dependence of Δ
n
ij
remains almost constant until the self-absorption becomes significant. The threshold condition for laser oscillation is discussed in relation to the calculated Δ
n
ij
. Laser oscillation is possible for the line pair (2, 3) at an electron density and temperature higher than for the other pairs (3, 4) and (4, 5) when self-absorption is negligible. |
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Bibliography: | ObjectType-Article-2 SourceType-Scholarly Journals-1 ObjectType-Feature-1 content type line 23 |
ISSN: | 0022-4073 1879-1352 |
DOI: | 10.1016/0022-4073(83)90133-4 |