1996
DOI: 10.1109/3.535355
|View full text |Cite
|
Sign up to set email alerts
|

A simplified analytic model for gain saturation and power extraction in the flowing chemical oxygen-iodine laser

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

2
17
0

Year Published

2001
2001
2022
2022

Publication Types

Select...
3
3
2

Relationship

0
8

Authors

Journals

citations
Cited by 47 publications
(19 citation statements)
references
References 5 publications
2
17
0
Order By: Relevance
“…For the study of unstable cavities, numerous models faithfully preserve the cavity geometry [8][9][10]. In cases of stable resonators, however, the Fabry-Perot cavity and the roof-top cavity are often used as the approximation model [3,[12][13][14]. The Fabry-Perot model was successful in estimating the output power and the chemical efficiency with respect to the outcoupling rate and the flow condition.…”
Section: Introductionmentioning
confidence: 99%
See 2 more Smart Citations
“…For the study of unstable cavities, numerous models faithfully preserve the cavity geometry [8][9][10]. In cases of stable resonators, however, the Fabry-Perot cavity and the roof-top cavity are often used as the approximation model [3,[12][13][14]. The Fabry-Perot model was successful in estimating the output power and the chemical efficiency with respect to the outcoupling rate and the flow condition.…”
Section: Introductionmentioning
confidence: 99%
“…However, certain difficulty arises when using the Fabry-Perot model to predict the intensity pattern. The upstream-downstream optical coupling effect in COIL with stable cavity, known as the sugar scooping phenomenon, cannot be explained by the Fabry-Perot model [3,[13][14]. In order to simulate this phenomenon, Yang adopted the roof-top cavity model which forces the optical field to flip as it is reflected by one of the mirrors [14].…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…The concentration of atomic iodine is about 3% of that of molecular oxygen and each iodine atom is repumped and cycled many times throughout the flow field during the lasing process. According to the assumptions made in 1) and 2), it can be obtained that n1+n2=n0, (1) n+n=[O2], (2) Proc. of SPIE Vol.…”
Section: Gain Saturation Equation Of the Sgk Model In Flowing Coilmentioning
confidence: 99%
“…The dissociation of iodine has occurred upstream of the laser cavity and deactivation in the cavity during the lasing process is negligible. It means that nl+n2=n, (1) where n1 and n2 are the population of the excited state I(2P3/2) and the ground state I(2P]/2) (or the upper and lower laser level) of the atomic iodine, respectively, n is the total particle number of the atomic iodine entering the laser cavity. The concentration of 02 C ) is assumed to be negligible.…”
Section: Fundamental Expressions In Coilmentioning
confidence: 99%