• Photonics Research
  • Vol. 13, Issue 4, 897 (2025)
Danqing Liu, Changlei Guo*, Chunzhao Ma, Weitong Fan..., Xuezhen Gong, Zhen Zhang, Wenxun Li, Jie Xu, Kui Liu and Hsien-Chi Yeh|Show fewer author(s)
Author Affiliations
  • MOE Key Laboratory of TianQin Mission, TianQin Research Center for Gravitational Physics & School of Physics and Astronomy, Frontiers Science Center for TianQin, CNSA Research Center for Gravitational Waves, Sun Yat-sen University (Zhuhai Campus), Zhuhai 519082, China
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    DOI: 10.1364/PRJ.543856 Cite this Article Set citation alerts
    Danqing Liu, Changlei Guo, Chunzhao Ma, Weitong Fan, Xuezhen Gong, Zhen Zhang, Wenxun Li, Jie Xu, Kui Liu, Hsien-Chi Yeh, "All-solid-state miniature laser gyroscope based on a single monolithic non-planar ring oscillator," Photonics Res. 13, 897 (2025) Copy Citation Text show less
    A typical NPRO geometry and its internal light paths. A, incident plane; B, C, D, total reflection planes; E, midpoint of BD; α, exterior incidence angle; β, dihedral angle.
    Fig. 1. A typical NPRO geometry and its internal light paths. A, incident plane; B, C, D, total reflection planes; E, midpoint of BD; α, exterior incidence angle; β, dihedral angle.
    (a) Schematic of the experimental setup for NPRO gyroscope. LD, laser diode; CM, collimator; DM, dichroic mirror; TEC, thermoelectric cooler; Att, optical attenuator; PD, photodetector. The current supply, temperature controllers, and electronics used for signal amplifying and filtering are not shown. (b) Spectrum of a typical beat signal at 346 kHz measured with resolution bandwidth (RBW) of 100 Hz.
    Fig. 2. (a) Schematic of the experimental setup for NPRO gyroscope. LD, laser diode; CM, collimator; DM, dichroic mirror; TEC, thermoelectric cooler; Att, optical attenuator; PD, photodetector. The current supply, temperature controllers, and electronics used for signal amplifying and filtering are not shown. (b) Spectrum of a typical beat signal at 346 kHz measured with resolution bandwidth (RBW) of 100 Hz.
    (a) Scheme of measuring wavefront distortion in NPRO; (b), (c) wavefront distortions measured with two different NPRO samples. The RMS and PV values are given.
    Fig. 3. (a) Scheme of measuring wavefront distortion in NPRO; (b), (c) wavefront distortions measured with two different NPRO samples. The RMS and PV values are given.
    Beat frequency noise comparison between beat signals from low-distortion (beat frequency at 328 kHz) and high-distortion (beat frequency at 334 kHz) NPRO samples.
    Fig. 4. Beat frequency noise comparison between beat signals from low-distortion (beat frequency at 328 kHz) and high-distortion (beat frequency at 334 kHz) NPRO samples.
    NPRO gyroscope beat frequency shift with different rotational speeds. The offset frequency is at 334 kHz.
    Fig. 5. NPRO gyroscope beat frequency shift with different rotational speeds. The offset frequency is at 334 kHz.
    Allan deviation of the NPRO gyroscope beat frequency.
    Fig. 6. Allan deviation of the NPRO gyroscope beat frequency.
    Noise investigations for the NPRO gyroscope. Red: beat frequency noise of the NPRO gyroscope in steady state; blue: magnetic noise measured with magnet in nominal position around the NPRO; gray: magnetic background noise measured when the magnet is removed; brown: NPRO temperature noise; green: pump power noise.
    Fig. 7. Noise investigations for the NPRO gyroscope. Red: beat frequency noise of the NPRO gyroscope in steady state; blue: magnetic noise measured with magnet in nominal position around the NPRO; gray: magnetic background noise measured when the magnet is removed; brown: NPRO temperature noise; green: pump power noise.
    (a) A conceptual package design of NPRO gyroscope with all optics and basic electronics. The body dimension of the package is 30 mm×25 mm×11 mm. (b) A new NPRO design with top and left views. The gain medium is Nd-glass. The purple line is the optical path. The dimension is 3 mm×13 mm×15 mm. (c) Projected bias instability versus scale factor (projected from Fig. 6). The black dashed line marks the Earth rotation speed; the blue and red points represent the bias instability achieved in the present experiment and the projected bias instability using the new NPRO sample under design, respectively.
    Fig. 8. (a) A conceptual package design of NPRO gyroscope with all optics and basic electronics. The body dimension of the package is 30  mm×25  mm×11  mm. (b) A new NPRO design with top and left views. The gain medium is Nd-glass. The purple line is the optical path. The dimension is 3  mm×13  mm×15  mm. (c) Projected bias instability versus scale factor (projected from Fig. 6). The black dashed line marks the Earth rotation speed; the blue and red points represent the bias instability achieved in the present experiment and the projected bias instability using the new NPRO sample under design, respectively.
    Modulation coefficient measurement results. (a) Beat frequency versus pump power; (b) beat frequency versus NPRO temperature; (c) beat frequency versus magnetic intensity. Red squares: measurements; black solid lines: linear fitting. The slopes and coefficients of determination R2 are given.
    Fig. 9. Modulation coefficient measurement results. (a) Beat frequency versus pump power; (b) beat frequency versus NPRO temperature; (c) beat frequency versus magnetic intensity. Red squares: measurements; black solid lines: linear fitting. The slopes and coefficients of determination R2 are given.
    ParameterIn ExperimentUnder DesignUnit
    Dimension3×8×123×13×15mm3
    AE10.510.5mm
    CE1.54.5mm
    α3050deg
    β901deg
    n1.821.54
    MaterialNd:YAG crystalNd-glass
    Scale factor38.1102.9Hz/(degs1)
    Table 1. NPRO Parameters in Experiment and under Design
    Danqing Liu, Changlei Guo, Chunzhao Ma, Weitong Fan, Xuezhen Gong, Zhen Zhang, Wenxun Li, Jie Xu, Kui Liu, Hsien-Chi Yeh, "All-solid-state miniature laser gyroscope based on a single monolithic non-planar ring oscillator," Photonics Res. 13, 897 (2025)
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