• Photonics Research
  • Vol. 9, Issue 9, 1715 (2021)
Robin Mevert1、2、*, Yuliya Binhammer1、2, Christian M. Dietrich1、2, Luise Beichert1、2, José R. Cardoso de Andrade1、2, Thomas Binhammer3, Jintao Fan1、2, and Uwe Morgner1、2
Author Affiliations
  • 1Institute of Quantum Optics, Leibniz University Hannover, Welfengarten 1, D-30167 Hannover, Germany
  • 2Cluster of Excellence PhoenixD, Welfengarten 1, D-30167 Hannover, Germany
  • 3neoLASE GmbH, Hollerithallee 17, D-30419 Hannover, Germany
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    DOI: 10.1364/PRJ.426107 Cite this Article Set citation alerts
    Robin Mevert, Yuliya Binhammer, Christian M. Dietrich, Luise Beichert, José R. Cardoso de Andrade, Thomas Binhammer, Jintao Fan, Uwe Morgner. Widely tunable, high-power, femtosecond noncollinear optical parametric oscillator in the visible spectral range[J]. Photonics Research, 2021, 9(9): 1715 Copy Citation Text show less
    Schematic setup of the VIS-NOPO. The upper part of the sketch shows the pump laser and the third-harmonic-generation setup. A pump lens L (f=200 mm) focuses the third harmonic into the Brewster-cut BBO crystal (θ=39°; L=2 mm), which is surrounded by two curved DCMs (M1andM2: d=25.4 mm; ROC=−150 mm) with a spectral transmission window at 345 nm. Moreover, a BK7 substrate (uncoated, L=3 mm) is inserted into the cavity, which consists of six additional plane DCMs (M3−M8) and an output coupling mirror (OC) with 14% transmission from 480 to 720 nm.
    Fig. 1. Schematic setup of the VIS-NOPO. The upper part of the sketch shows the pump laser and the third-harmonic-generation setup. A pump lens L (f=200  mm) focuses the third harmonic into the Brewster-cut BBO crystal (θ=39°; L=2  mm), which is surrounded by two curved DCMs (M1andM2: d=25.4  mm; ROC=150  mm) with a spectral transmission window at 345 nm. Moreover, a BK7 substrate (uncoated, L=3  mm) is inserted into the cavity, which consists of six additional plane DCMs (M3M8) and an output coupling mirror (OC) with 14% transmission from 480 to 720 nm.
    Tuning behavior of the VIS-NOPO. (a) Measured power spectral density (PSD) as a function of wavelength and cavity length/group delay. The green line indicates the calculated net intracavity GDD. (b) Measured pulse durations and output powers.
    Fig. 2. Tuning behavior of the VIS-NOPO. (a) Measured power spectral density (PSD) as a function of wavelength and cavity length/group delay. The green line indicates the calculated net intracavity GDD. (b) Measured pulse durations and output powers.
    (a) Normalized signal spectra for different cavity lengths. (b) Measured pulse durations (circles) and calculated Fourier limits (triangles). (c) Green line: calculated GDD.
    Fig. 3. (a) Normalized signal spectra for different cavity lengths. (b) Measured pulse durations (circles) and calculated Fourier limits (triangles). (c) Green line: calculated GDD.
    Measured slope efficiency and threshold of the signal at 530 nm. The solid red line illustrated a linear fit. Inset: signal beam profile at maximum output power.
    Fig. 4. Measured slope efficiency and threshold of the signal at 530 nm. The solid red line illustrated a linear fit. Inset: signal beam profile at maximum output power.
    (a) Long-term stability measurement of the signal output power. (b) Phase noise PSD of signal and pump.
    Fig. 5. (a) Long-term stability measurement of the signal output power. (b) Phase noise PSD of signal and pump.
    Robin Mevert, Yuliya Binhammer, Christian M. Dietrich, Luise Beichert, José R. Cardoso de Andrade, Thomas Binhammer, Jintao Fan, Uwe Morgner. Widely tunable, high-power, femtosecond noncollinear optical parametric oscillator in the visible spectral range[J]. Photonics Research, 2021, 9(9): 1715
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