• Photonics Research
  • Vol. 6, Issue 4, 238 (2018)
Mulong Liu1、2, Leiran Wang1、2、*, Qibing Sun1, Siqi Li1、2, Zhiqiang Ge1、2, Zhizhou Lu1、2, Weiqiang Wang1、2, Guoxi Wang1、2, Wenfu Zhang1、2、3, Xiaohong Hu1, and Wei Zhao1、2
Author Affiliations
  • 1State Key Laboratory of Transient Optics and Photonics, Xi’an Institute of Optics and Precision Mechanics (XIOPM), Chinese Academy of Sciences (CAS), Xi’an 710119, China
  • 2University of Chinese Academy of Sciences, Beijing 100049, China
  • 3e-mail: wfuzhang@opt.ac.cn
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    DOI: 10.1364/PRJ.6.000238 Cite this Article Set citation alerts
    Mulong Liu, Leiran Wang, Qibing Sun, Siqi Li, Zhiqiang Ge, Zhizhou Lu, Weiqiang Wang, Guoxi Wang, Wenfu Zhang, Xiaohong Hu, Wei Zhao. Influences of multiphoton absorption and free-carrier effects on frequency-comb generation in normal dispersion silicon microresonators[J]. Photonics Research, 2018, 6(4): 238 Copy Citation Text show less

    Abstract

    We investigate frequency-comb generation in normal dispersion silicon microresonators from the near-infrared to mid-infrared wavelength range in the presence of multiphoton absorption and free-carrier effects. It is found that parametric oscillation is inhibited in the telecom wavelength range resulting from strong two-photon absorption. On the contrary, beyond the wavelength of 2200 nm, where three- and four-photon absorption are less detrimental, a comb can be generated with moderate pump power, or free-carriers are swept out by a positive-intrinsic-negative structure. In the temporal domain, the generated combs correspond to flat-top pulses, and the pulse duration can be easily controlled by varying the laser detuning. The reported comb generation process shows a high conversion efficiency compared with anomalous dispersion regime, which can guide and promote comb formation in materials with normal dispersion. As the comb spectra cover the mid-infrared wavelength range, they can find applications in comb-based radiofrequency photonic filters and mid-infrared spectroscopy.
    TRE(t,τ)t={α2κ2iδ0+iLβ22!(iτ)2+(1+iω0τ)×[iγL|E(t,τ)|2β2PAL2Aeff|E(t,τ)|2β3PAL3Aeff2|E(t,τ)|4β4PAL4Aeff3|E(t,τ)|6]σL2(1+iμ)Nc(t,τ)}E(t,τ)+κEin,(1a)

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    Ein=Pin1+Pin2exp(i2πfτ),(1b)

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    dNc(t)dt=β2PA2ω|E|4Aeff2+β3PA3ω|E|6Aeff3+β4PA4ω|E|8Aeff4Nc(t)τeff,(1c)

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    Mulong Liu, Leiran Wang, Qibing Sun, Siqi Li, Zhiqiang Ge, Zhizhou Lu, Weiqiang Wang, Guoxi Wang, Wenfu Zhang, Xiaohong Hu, Wei Zhao. Influences of multiphoton absorption and free-carrier effects on frequency-comb generation in normal dispersion silicon microresonators[J]. Photonics Research, 2018, 6(4): 238
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