TY - JOUR
T1 - Spectrally-isolated violet to blue wavelength generation by cascaded degenerate four-wave mixing in a photonic crystal fiber
AU - Yuan, Jinhui
AU - Kang, Zhe
AU - Li, Feng
AU - Zhang, Xianting
AU - Zhou, Guiyao
AU - Sang, Xinzhu
AU - Wu, Qiang
AU - Yan, Binbin
AU - Zhou, Xian
AU - Wang, Liang
AU - Zhong, Kangping
AU - Wang, Kuiru
AU - Yu, Chongxiu
AU - Tam, Hwa Yaw
AU - Wai, P. K.A.
N1 - Publisher Copyright:
© 2016 Optical Society of America.
PY - 2016/6/1
Y1 - 2016/6/1
N2 - Generation of spectrally-isolated wavelengths in the violet to blue region based on cascaded degenerate four-wave mixing (FWM) is experimentally demonstrated for the first time in a tailor-made photonic crystal fiber, which has two adjacent zero dispersion wavelengths (ZDWs) at 696 and 852 nm in the fundamental mode. The influences of the wavelength λp and the input average power Pav of the femtosecond pump pulses on the phase-matched frequency conversion process are studied. When femtosecond pump pulses at λp of 880, 870, and 860 nm and Pav of 500 mW are coupled into the normal dispersion region close to the second ZDW, the first anti-Stokes waves generated near the first ZDW act as a secondary pump for the next FWM process. The conversion efficiency ηas2 of the second anti-Stokes waves, which are generated at the violet to blue wavelengths of 430, 456, and 472 nm, are 4.8, 6.48, and 9.66%, for λp equalling 880, 870, and 860 nm, respectively.
AB - Generation of spectrally-isolated wavelengths in the violet to blue region based on cascaded degenerate four-wave mixing (FWM) is experimentally demonstrated for the first time in a tailor-made photonic crystal fiber, which has two adjacent zero dispersion wavelengths (ZDWs) at 696 and 852 nm in the fundamental mode. The influences of the wavelength λp and the input average power Pav of the femtosecond pump pulses on the phase-matched frequency conversion process are studied. When femtosecond pump pulses at λp of 880, 870, and 860 nm and Pav of 500 mW are coupled into the normal dispersion region close to the second ZDW, the first anti-Stokes waves generated near the first ZDW act as a secondary pump for the next FWM process. The conversion efficiency ηas2 of the second anti-Stokes waves, which are generated at the violet to blue wavelengths of 430, 456, and 472 nm, are 4.8, 6.48, and 9.66%, for λp equalling 880, 870, and 860 nm, respectively.
UR - http://www.scopus.com/inward/record.url?scp=84975090503&partnerID=8YFLogxK
U2 - 10.1364/OL.41.002612
DO - 10.1364/OL.41.002612
M3 - Journal article
AN - SCOPUS:84975090503
SN - 0146-9592
VL - 41
SP - 2612
EP - 2615
JO - Optics Letters
JF - Optics Letters
IS - 11
ER -