TY - JOUR
T1 - Continuous-wave multifrequency laser emission generated through stimulated Raman scattering and four-wave Raman mixing in an optical cavity
AU - Zaitsu, Shin Ichi
AU - Imasaka, Totaro
N1 - Funding Information:
Manuscript received February 18, 2011; revised May 22, 2011; accepted May 10, 2011. Date of current version July 14, 2011. This work was supported in part by the PRESTO Program of the Japan Science and Technology Agency, Grants-in-Aid for Scientific Research, and the Global COE Program “Science for Future Molecular Systems” from the Ministry of Education, Culture, Science, Sports and Technology of Japan.
PY - 2011
Y1 - 2011
N2 - The frequency of a continuous-wave laser was converted via high-order stimulated Raman scattering and four-wave Raman mixing in a high-finesse optical cavity. The threshold for the generation of a Stokes beam was determined by the Raman gain coefficient and the loss in the cavity. The intracavity power of the second-order Stokes beam increased with an increase in pump power, whereas the power of the first-order Stokes beam stayed constant. The output power of the anti-Stokes beam was low when there was a phase mismatch between the pump and the first-order Stokes beam. The anti-Stokes beam, however, was enhanced by decreasing the pressure of the Raman active medium. This suggests that the dispersion can be used to improve the efficiency of the intracavity four-wave Raman mixing.
AB - The frequency of a continuous-wave laser was converted via high-order stimulated Raman scattering and four-wave Raman mixing in a high-finesse optical cavity. The threshold for the generation of a Stokes beam was determined by the Raman gain coefficient and the loss in the cavity. The intracavity power of the second-order Stokes beam increased with an increase in pump power, whereas the power of the first-order Stokes beam stayed constant. The output power of the anti-Stokes beam was low when there was a phase mismatch between the pump and the first-order Stokes beam. The anti-Stokes beam, however, was enhanced by decreasing the pressure of the Raman active medium. This suggests that the dispersion can be used to improve the efficiency of the intracavity four-wave Raman mixing.
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U2 - 10.1109/JQE.2011.2159362
DO - 10.1109/JQE.2011.2159362
M3 - Article
AN - SCOPUS:79960657196
SN - 0018-9197
VL - 47
SP - 1129
EP - 1135
JO - IEEE Journal of Quantum Electronics
JF - IEEE Journal of Quantum Electronics
IS - 8
M1 - 5873113
ER -