Photonics Research, Volume. 12, Issue 9, 2012(2024)

Frequency comb generation from the ultraviolet to mid-infrared region based on a three-stage cascaded PPLN chain Editors' Pick

Xiong Qin1、†, Daping Luo1、†, Lian Zhou1,2、*, Jiayi Pan1, Zejiang Deng1, Gehui Xie1, Chenglin Gu1, and Wenxue Li1,3、*
Author Affiliations
  • 1State Key Laboratory of Precision Spectroscopy, East China Normal University, Shanghai 200062, China
  • 2e-mail: lzhou@lps.ecnu.edu.cn
  • 3e-mail: wxli@phy.ecnu.edu.cn
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    Figures & Tables(6)
    Schematic of offset-free frequency comb covering the UV-to-MIR region. HNLF: high nonlinear fiber; PPLN WG: periodically poled lithium niobate waveguide; DFG: difference frequency generation; Ge: AR-coated germanium plate; BPF: MIR bandpass filter; YDFA: Yb-doped fiber amplifier; OPA: optical parametric amplification; OPM: off-axis parabolic mirror; HHG: high-order harmonic generation; H2–H8: frequency components of harmonics. The H2–H4 and H5–H8 were respectively observed on an infrared detector card and a white paper.
    (a) Injected spectrum (yellow line) and expanding SCG (blue line). (b) Visible–MIR spectrum emitted from DFG (measurement devices: Ocean Optics HR4000, Yokogawa AQ6370, and Bristol 771B).
    (a) NIR pump spectrum of OPA. (b) Calculated signal/idler profiles and corresponding periods with pump wavelengths at 1.025, 1.050, and 1.075 μm. (c) Spectrum of the signal light filtered from the comb source. Spectra from the OPAs using (d) a fan-out crosswise-poled PPLN crystal (OPA1) and (e) an axial-poled CPPLN waveguide (OPA2).
    (a) Average power of amplified MIR light after OPA1 and OPA2. (b) Pump-to-signal conversion efficiency as a function of average pump power.
    HHG spectral components of H1–H10 harmonics separately driven by MIR combs of (a) OPA1 and (b) OPA2. S1, S2, S3, and S4 represent four optical spectrometers, specifically corresponding to the models of Bristol 771B, Yokogawa AQ6375E, Yokogawa AQ6370, and Ocean Optics HR4000.
    • Table 1. Output Powers of the Generated Harmonic Components Using OPA1 and OPA2

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      Table 1. Output Powers of the Generated Harmonic Components Using OPA1 and OPA2

      OPA1OPA2
      HHGWavelengthOutput PowerPower MeterHHGWavelengthOutput PowerPower Meter
      H13157–3722 nm30.12 mWThorlabs S405CH13061–4027 nm20.24 mWThorlabs S405C
      H21402–1775 nm24.29 mWThorlabs S122CH21449–2040 nm13.62 mW
      H3984–1322 nm12.26 mWH3775–1316 nm11.54 mW
      H4829–909 nm4.61 mWH4
      H5634–700 nm0.42 mWThorlabs S120VCH5440–750 nm1.18 mW
      H6532–596 nm0.73 mWH6
      H7467–508 nm40.41 μWH7
      H8411–452 nm30.26 μWH8
      H9375–388 nm5.42 μWH9384–407 nm3.42 μWThorlabs S120VC
      H10353–361 nm1.05 μWH10354–369 nm0.92 μW
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    Xiong Qin, Daping Luo, Lian Zhou, Jiayi Pan, Zejiang Deng, Gehui Xie, Chenglin Gu, Wenxue Li, "Frequency comb generation from the ultraviolet to mid-infrared region based on a three-stage cascaded PPLN chain," Photonics Res. 12, 2012 (2024)

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    Paper Information

    Category: Instrumentation and Measurements

    Received: May. 6, 2024

    Accepted: Jun. 17, 2024

    Published Online: Aug. 28, 2024

    The Author Email: Lian Zhou (lzhou@lps.ecnu.edu.cn), Wenxue Li (wxli@phy.ecnu.edu.cn)

    DOI:10.1364/PRJ.528880

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