• Chinese Journal of Lasers
  • Vol. 45, Issue 4, 400001 (2018)
Lu Qiao1、2, Shi Lei1, and Mao Qinghe1、2、*
Author Affiliations
  • 1[in Chinese]
  • 2[in Chinese]
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    DOI: 10.3788/CJL201845.0400001 Cite this Article Set citation alerts
    Lu Qiao, Shi Lei, Mao Qinghe. Research Advances in Dual-Comb Spectroscopy[J]. Chinese Journal of Lasers, 2018, 45(4): 400001 Copy Citation Text show less
    (a) Time domain and frequency domain diagrams for pulse electric field of ideal mode-locking laser; (b) three typical locking schemes for OFCs
    Fig. 1. (a) Time domain and frequency domain diagrams for pulse electric field of ideal mode-locking laser; (b) three typical locking schemes for OFCs
    (a) Schematic for actively measuring principle of OFC-based FTS[25]; (b) schematic for DCS measuring principle[25]; (c) asynchronous optical sampling and measuring process in time domain; (d) multiheterodyne in frequency domain for measuring process of DCS
    Fig. 2. (a) Schematic for actively measuring principle of OFC-based FTS[25]; (b) schematic for DCS measuring principle[25]; (c) asynchronous optical sampling and measuring process in time domain; (d) multiheterodyne in frequency domain for measuring process of DCS
    Configuration of OFC locked with optical frequency reference scheme[24]
    Fig. 3. Configuration of OFC locked with optical frequency reference scheme[24]
    (a) Configuration of coherent DCS[36]; (b) measured phase and transmission spectra for HCN sample[36];(c) local zoom near 195 THz in Fig.4(b), measured phase (green curve) and transmission spectra (black curve) agree well with theoretical results (dotted blue line, and offset by 0.1 rad) calculated from absorption data through Kramers-Kronig relation[36]
    Fig. 4. (a) Configuration of coherent DCS[36]; (b) measured phase and transmission spectra for HCN sample[36];(c) local zoom near 195 THz in Fig.4(b), measured phase (green curve) and transmission spectra (black curve) agree well with theoretical results (dotted blue line, and offset by 0.1 rad) calculated from absorption data through Kramers-Kronig relation[36]
    (a) Experimental site layout of open-path multicomponent greenhouse gas online measurements with coherent DCS[59]; (b) comparison of results of greenhouse gases measured by coherent DCS with those calculated with HITRAN database[59]; (c) photograph of vehicle-borne OFC[61]
    Fig. 5. (a) Experimental site layout of open-path multicomponent greenhouse gas online measurements with coherent DCS[59]; (b) comparison of results of greenhouse gases measured by coherent DCS with those calculated with HITRAN database[59]; (c) photograph of vehicle-borne OFC[61]
    (a) Adaptive DCS scheme based on tracking-recording error signal technique with FBG[37]; (b) measured results with adaptive DCS[37]
    Fig. 6. (a) Adaptive DCS scheme based on tracking-recording error signal technique with FBG[37]; (b) measured results with adaptive DCS[37]
    (a) Schematic of adaptive DCS based on CW laser references[22]; (b) comparison of C2H2 absorption spectra respectively measured by constant and adaptive clocks sampling with those obtained by using HITRAN database[22]
    Fig. 7. (a) Schematic of adaptive DCS based on CW laser references[22]; (b) comparison of C2H2 absorption spectra respectively measured by constant and adaptive clocks sampling with those obtained by using HITRAN database[22]
    Configuration and measuring principle of DCS scheme based on single OFC with repetition rate tuned and time-delay-multiplexing technique[27]. (a) Configuration; (b) measuring principle
    Fig. 8. Configuration and measuring principle of DCS scheme based on single OFC with repetition rate tuned and time-delay-multiplexing technique[27]. (a) Configuration; (b) measuring principle
    (a) DCS based on single laser source with dual-output ports extract lights respectively propagating in different directions inside cavity[57]; (b) DCS with dual-wavelength mode-locked fiber laser[30]
    Fig. 9. (a) DCS based on single laser source with dual-output ports extract lights respectively propagating in different directions inside cavity[57]; (b) DCS with dual-wavelength mode-locked fiber laser[30]
    Operation principles and realization schemes for improving spectral resolution of DCS with (a) phase-modulated pulse technique[66]and (b) spectral interleave scheme[69]
    Fig. 10. Operation principles and realization schemes for improving spectral resolution of DCS with (a) phase-modulated pulse technique[66]and (b) spectral interleave scheme[69]
    Measureable wavebands and spectral ranges for DCS published
    Fig. 11. Measureable wavebands and spectral ranges for DCS published
    Coherent Raman DCS and its measured spectral and imaging results[75]
    Fig. 12. Coherent Raman DCS and its measured spectral and imaging results[75]
    DCSNEA /(cm-1·Hz-1/2)FSNR /(Hz1/2)SNRResolution /GHzSpectrum coverage
    CE-DCS[73]1×10-104.6×105380@18 μs4.50020 nm@1040 nm
    CE-OE-DCS[72]1.5×10-82.9×104189@320 s0.20350 GHz@1550 nm
    OP-DCS[59]7.3×10-101.4×106588@300 s0.10032 nm@1620 nm
    LA-DCS[23]2.2×10-72.3×108316000@24 h0.10018 THz@1560 nm
    A-DCS[22]4.2×10-71.25×10720@467 μs1.10014.5 THz@1560 nm
    OPO-DCS[74]5.3×10-75.3×10681@720 μs6.00010.5 THz@3 μm
    Raman-DCS[75]2×10-61.8×1071000@296 μs120.00042 THz@12 μm
    OE-DCS[35]1.7×10-91.3×1062600@52 ms0.30035 GHz@1550 nm
    MC-DCS[34]2.5×10-73×10674@20 μs22.0004 THz@1550 nm
    Table 1. Performance indexes for reported DCS