Abstract
Enhancements in the output energy of an XeCl laser of more than 50 percent have been observed by Injecting 2–43 mJ of 308 nm laser radiation into the resonator 10–150 ns prior to the emergence of the final XeCl pulse. This effect is a strong function of the time delay (Δt) between the two lasers and is most pronounced when the injected (external) pulse precedes the XeCl laser pulse by 45 ns. For| Δt| ≤ 100 ns, the external radiation appears to be simply “seeding” the XeCl laser cavity which allows the second laser to reach threshold earlier and thereby improve its extraction efficiency. For 100 ≤ |Δt| ≤ 150 ns, the enhancement may to arise from the depletion of the number density of an impurity molecule which absorbs strongly at 308 nm.
Original language | English (US) |
---|---|
Pages (from-to) | 501-504 |
Number of pages | 4 |
Journal | IEEE Journal of Quantum Electronics |
Volume | 22 |
Issue number | 4 |
DOIs | |
State | Published - Apr 1986 |
Fingerprint
ASJC Scopus subject areas
- Atomic and Molecular Physics, and Optics
- Condensed Matter Physics
- Electrical and Electronic Engineering
Cite this
XeCl Laser Power Enhancement with an External Ultraviolet Laser. / Geohegan, D. B.; Eden, James Gary; McCown, A. W.
In: IEEE Journal of Quantum Electronics, Vol. 22, No. 4, 04.1986, p. 501-504.Research output: Contribution to journal › Article
}
TY - JOUR
T1 - XeCl Laser Power Enhancement with an External Ultraviolet Laser
AU - Geohegan, D. B.
AU - Eden, James Gary
AU - McCown, A. W.
PY - 1986/4
Y1 - 1986/4
N2 - Enhancements in the output energy of an XeCl laser of more than 50 percent have been observed by Injecting 2–43 mJ of 308 nm laser radiation into the resonator 10–150 ns prior to the emergence of the final XeCl pulse. This effect is a strong function of the time delay (Δt) between the two lasers and is most pronounced when the injected (external) pulse precedes the XeCl laser pulse by 45 ns. For| Δt| ≤ 100 ns, the external radiation appears to be simply “seeding” the XeCl laser cavity which allows the second laser to reach threshold earlier and thereby improve its extraction efficiency. For 100 ≤ |Δt| ≤ 150 ns, the enhancement may to arise from the depletion of the number density of an impurity molecule which absorbs strongly at 308 nm.
AB - Enhancements in the output energy of an XeCl laser of more than 50 percent have been observed by Injecting 2–43 mJ of 308 nm laser radiation into the resonator 10–150 ns prior to the emergence of the final XeCl pulse. This effect is a strong function of the time delay (Δt) between the two lasers and is most pronounced when the injected (external) pulse precedes the XeCl laser pulse by 45 ns. For| Δt| ≤ 100 ns, the external radiation appears to be simply “seeding” the XeCl laser cavity which allows the second laser to reach threshold earlier and thereby improve its extraction efficiency. For 100 ≤ |Δt| ≤ 150 ns, the enhancement may to arise from the depletion of the number density of an impurity molecule which absorbs strongly at 308 nm.
UR - http://www.scopus.com/inward/record.url?scp=0022700906&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=0022700906&partnerID=8YFLogxK
U2 - 10.1109/JQE.1986.1073002
DO - 10.1109/JQE.1986.1073002
M3 - Article
AN - SCOPUS:0022700906
VL - 22
SP - 501
EP - 504
JO - IEEE Journal of Quantum Electronics
JF - IEEE Journal of Quantum Electronics
SN - 0018-9197
IS - 4
ER -