TY - GEN
T1 - Improvement of four wave mixing efficiency in DSF by clock pumping
AU - Yang, Aiying
AU - Qiao, Yaojun
AU - Sun, Yunan
PY - 2007
Y1 - 2007
N2 - In this paper, we investigate utilizing clock modulated signal as a pump to improve the efficiency of FWM in 26.5km dispersion shifted fiber. The experimental results show that, with the clock pumping, the conjugated FWM component has higher intensity than that with the CW pumping. The reason behind it is that SBS process is greatly quenched with the clock pumping, so most power of the pumping light contributes to nonlinear interaction with the probe signal during the propagation through DSF. But for CW pumping greater than Brillouin threshold, most power is depleted by SBS process and converted to backward Stokes light, so less power is left for other nonlinear process such as SPM, XPM and FWM to take place. As a result, the FWM components have lower intensity, and the pump and probe signal spectrum is also much less broadened. The measurement shows that, the improvement of FWM efficiency is negligible when the pump power is less than 10dBm. But when the pump power is greater than about 11dBm, the improvement becomes significant and increases with the increased pump power. When pump power reaches 17dBm, the improvement is increased to about 9dB.
AB - In this paper, we investigate utilizing clock modulated signal as a pump to improve the efficiency of FWM in 26.5km dispersion shifted fiber. The experimental results show that, with the clock pumping, the conjugated FWM component has higher intensity than that with the CW pumping. The reason behind it is that SBS process is greatly quenched with the clock pumping, so most power of the pumping light contributes to nonlinear interaction with the probe signal during the propagation through DSF. But for CW pumping greater than Brillouin threshold, most power is depleted by SBS process and converted to backward Stokes light, so less power is left for other nonlinear process such as SPM, XPM and FWM to take place. As a result, the FWM components have lower intensity, and the pump and probe signal spectrum is also much less broadened. The measurement shows that, the improvement of FWM efficiency is negligible when the pump power is less than 10dBm. But when the pump power is greater than about 11dBm, the improvement becomes significant and increases with the increased pump power. When pump power reaches 17dBm, the improvement is increased to about 9dB.
KW - Continue wave light
KW - Dispersion shifted fiber
KW - Four wave mixing
KW - Stimulated Brilliouin scattering
KW - Wavelength conversion
UR - http://www.scopus.com/inward/record.url?scp=42549156310&partnerID=8YFLogxK
U2 - 10.1117/12.745355
DO - 10.1117/12.745355
M3 - Conference contribution
AN - SCOPUS:42549156310
SN - 9780819469441
T3 - Proceedings of SPIE - The International Society for Optical Engineering
BT - Passive Components and Fiber-based Devices IV
T2 - Passive Components and Fiber-based Devices IV
Y2 - 2 November 2007 through 5 November 2007
ER -