1979
DOI: 10.1016/0030-4018(79)90281-5
|View full text |Cite
|
Sign up to set email alerts
|

Pulse compression in continuously pumped dye lasers with a slow saturable absorber

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1

Citation Types

0
1
0

Year Published

1981
1981
1983
1983

Publication Types

Select...
3
1

Relationship

0
4

Authors

Journals

citations
Cited by 4 publications
(1 citation statement)
references
References 6 publications
0
1
0
Order By: Relevance
“…One can set up a model cavity (either a two-way configuration or a ring as shown in figure 42(6)) with amplifying and absorbing elements at arbitrary positions and readily obtain, at a particular point in the circuit, the unique value of J that repeats itself on successive transits (New 1972, Muller 1979). However, it is mathematically more convenient to adopt the ring cavity model of figure 42(a), in which case it is readily shown from equations (6.1)-( 6.3) that J is the root of the equation ( New where subscripts L and T denote values of A and B presented to the leading and trailing edges of the pulses, respectively.…”
Section: Transitsmentioning
confidence: 99%
“…One can set up a model cavity (either a two-way configuration or a ring as shown in figure 42(6)) with amplifying and absorbing elements at arbitrary positions and readily obtain, at a particular point in the circuit, the unique value of J that repeats itself on successive transits (New 1972, Muller 1979). However, it is mathematically more convenient to adopt the ring cavity model of figure 42(a), in which case it is readily shown from equations (6.1)-( 6.3) that J is the root of the equation ( New where subscripts L and T denote values of A and B presented to the leading and trailing edges of the pulses, respectively.…”
Section: Transitsmentioning
confidence: 99%