Vernier spectrometer using counter-propagating soliton microcombs

Vernier spectrometer using counter-propagating soliton microcombs

Qi-Fan Yang, Boqiang Shen, Heming Wang, Minh Tran, Zhewei Zhang, Ki Youl Yang, Lue Wu, Chengying Bao, John Bowers, Amnon Yariv and Kerry Vahala
T. J. Watson Laboratory of Applied Physics, California Institute of Technology, Pasadena, California 91125, USA.
University of California, Santa Barbara, Department of Electrical and Computer Engineering, Santa Barbara, CA 93106, USA.
These authors contributed equally to this work.
Corresponding author:
July 20, 2019

Acquisition of laser frequency with high resolution under continuous and abrupt tuning conditions is important for sensing, spectroscopy and communications. Here, a single microresonator provides rapid and broad-band measurement of frequencies across the optical C-band with a relative frequency precision comparable to conventional dual frequency comb systems. Dual-locked counter-propagating solitons having slightly different repetition rates are used to implement a Vernier spectrometer. Laser tuning rates as high as 10 THz/s, broadly step-tuned lasers, multi-line laser spectra and also molecular absorption lines are characterized using the device. Besides providing a considerable technical simplification through the dual-locked solitons and enhanced capability for measurement of arbitrarily tuned sources, this work reveals possibilities for chip-scale spectrometers that greatly exceed the performance of table-top grating and interferometer-based devices.

Frequency-agile lasers are ubiquitous in sensing, spectroscopy and optical communications wilner2008communications (); allen1998diode (); choma2003sensitivity () and measurement of their optical frequency for tuning and control is traditionally performed by grating and interferometer-based spectrometers, but more recently these measurements can make use of optical frequency combsjones2000carrier (); holzwarth2000optical (); diddams2010evolving (). Frequency combs provide a remarkably stable measurement grid against which optical signal frequencies can be determined subject to the ambiguity introduced by their equally spaced comb lines. The ambiguity can be resolved for continuously frequency swept signals by counting comb teeth del2009frequency () relative to a known comb tooth; and this method has enabled measurement of remarkably high chirp rates coddington2012characterizing (). However, signal sources can operate with abrupt frequency jumps so as to quickly access a new spectral region or for switching purposes, and this requires a different approach. In this case, a second frequency comb with a different comb line spacing can provide a Vernier scale giorgetta2010fast () for comparison with the first comb to resolve the ambiguity under quite general tuning conditions ma2003new (); peng2008optical (); giorgetta2010fast (). This Vernier concept is also used in dual comb spectroscopycoddington2016dual (); suh2016microresonator (), but in measuring active signals the method can be significantly enhanced to quickly identify signal frequencies through a signal correlation technique giorgetta2010fast (). The power of the Vernier-based method relies upon mapping of optical comb frequencies into a radio-frequency grid of frequencies, the precision of which is set by the relative line-by-line frequency stability of the two frequency combs. This stability can be guaranteed by self-referencing each comb using a common high-stability radio-frequency source or through optical locking of each comb to reference lasers whose relative stability is ensured by mutual locking to a common optical cavity.

Figure 1: Spectrometer concept, experimental setup and static measurement. (A) Counter propagating soliton frequency combs (red and blue) feature repetition rates that differ by . Their propagation in the resonator causes phase-locking at the comb line with index . Also, the comb teeth separated by at are derived from a single pump laser and therefore also are effectively locked. This dual locking of the vernier-like comb frequencies enables precise measurement of a laser (green) at frequency when combined with electrical correlation of the comb signals to determine . Once calibrated, the tunable laser can resolve chemical absorption lines (grey) with high precision. (B) Experimental setup. AOM: acousto-optic modulator; CIRC: circulator; PD: photodetector. Supplement includes more detail. Inset: scanning electron microscope image of a silica resonator. (C) Typical measured spectrum of used to determine order . For this spectrum: = 2.8052 MHz and kHz giving . (D) The spectrograph of the dual soliton interferogram (pseudo color). Line spacing gives kHz. White squares correspond to the index in panel C. (E) Optical spectra of counter-propagating solitons. Pumps are filtered and denoted by dashed lines.(F) Measured wavelength of an external cavity diode laser operated in steady state. (G) Residual deviations between ECDL laser frequency measurement as given by the MSS and a wavemeter. Error bars give the systematic uncertainty as limited by the reference laser in panel B.

Here, a broad-band, high-resolution Vernier soliton microcomb spectrometer is demonstrated using a single miniature comb device that generates two mutually-phase-locked combs. The principle of operation relies upon an optical phase locking effect observed in the generation of counter-propagating solitons within high-Q whispering gallery resonators yang2017counter (). Soliton generation in microcavities is being studied for miniaturization to the chip-scale of complete comb systems Kippenberg2018 () and these so-called soliton microcombs have now been demonstrated in a wide range of microcavity systems herr2014temporal (); yi2015soliton (); brasch2016photonic (); wang2016intracavity (); joshi2016thermally (); gong2018high (). In the counter-propagating soliton system, it is found that the clockwise (cw) and counter-clockwise (ccw) comb frequencies can be readily phase locked with distinct repetition rates that are also locked. This mutual double-locking creates line-by-line relative frequency stability for the underlying microcomb spectra that is more characteristic of fully self-referenced dual comb systems. The resulting Vernier of comb frequencies in the optical domain maps to an exceptionally stable radio frequency grid. Application of the signal correlation method giorgetta2010fast () to this system, then enables a microresonator soliton spectrometer (MSS) for rapid and high accuracy measurement of frequency.

To establish its performance and for comparison with dual fiber-mode-locked-laser spectrometers giorgetta2010fast () the MSS is applied to measure a 10 THz/s laser frequency chirping rate, step tuning of a laser, as well as acquisition of high-resolution molecular vibronic spectra over the optical C-band. Moreover, a method for signal frequency extraction is developed that uses the high relative stability of the cw and ccw combs to unambiguously determine frequencies in complex spectra containing 100s of frequencies.

Figure 2: Laser tuning and spectroscopy measurements. (A) Measurement of a rapidly tuning laser showing index (upper), instantaneous frequency (middle), and higher resolution plot of wavelength relative to average linear rate (lower), all plotted versus time. (B) Measurement of a broadband step-tuned laser as for laser in panel A. Lower panel is a zoom-in to illustrate resolution of the measurement. (C) Spectroscopy of HCN gas. A vibronic level of HCN gas at 5 Torr is resolved using the laser in panel A. (D) Energy level diagram showing transitions between ground state and 2 levels. The measured (reference) transition wavenumbers are noted in red (blue).
Figure 3: Measurement of a fiber mode-locked laser (A) Pulse trains generated from a fiber mode-locked laser (FMLL) are sent into an optical spectral analyzer (OSA) and the MSS. (B) Optical spectrum of the FMLL measured by the OSA. (C) Optical spectrum of the FMLL measured using the MSS. Only a 60-GHz wavelength range is selected. (D) Measured (blue) and fitted (red) FMLL mode frequencies versus index. The slope of the fitted line is set to 249.7 MHz, the measured FMLL repetition rate. (E) Residual MSS deviation between measurement and fitted value.

The measurement concept in the frequency domain is depicted in Fig. 1A where comb spectra from doubled-locked cw and ccw solitons are shown. The solitons are pumped from a single laser source that is modulated as shown in figure 1B to produce the two mutually-coherent pump lines at order with frequency separation . The difference in pumping frequencies (MHz range) causes the soliton repetition rates to differ by which sets up a vernier effect in the respective soliton comb frequencies. As detailed elsewhere, the cw and ccw combs will experience frequency locking at order for certain pumping frequencies yang2017counter (). This locking requires that . Also, because the two pump frequencies are derived from a single laser source and have a high relative frequency stability ( is very stable), the two combs are also effectively locked at order . The order can readily increased or decreased by adjusting . The line-by-line relative frequency stability caused by this double locking is comparable to an excellent radio-frequency source. Moreover, the frequency spacings between comb tooth pairs occur at precise integer multiples of (the stability of which is ensured through the relation ), and thereby creates an extremely stable optical frequency vernier for mapping of the comb spectra into a radio frequency grid spectrum.

The spectrometer operates as follows. A test laser frequency is measured using either of the following expressions: where is the comb order nearest to the laser frequency, are the comb repetition rates, are the heterodyne beat frequencies of the test laser with the two frequency comb teeth at order , and is the frequency at . Comb repetition rates and the beats are measured by co-detection of the combs and the test laser to produce the electrical signals in Fig. 1B. The correlation method giorgetta2010fast () is used to determine . This method can be understood as a calculation of the frequency difference by formation of followed by fast Fourier transform (FFT). A typical FFT spectrum of is shown in Fig. 1C and gives a spectral line at . To determine requires which is measured by heterodyne of the solitons to produce electrical signal . Figure 1D is a narrow frequency span of the FFT of and shows how the optical frequency vernier is mapped into a stable radio-frequency grid with line spacing . The order corresponding to the FFT of the signal (Fig. 1C spectrum) is also indicated. These steps are performed automatically to provide a real time measurement of relative to . To determine the order of a comb tooth nearest a reference laser (with known and stable frequency) is determined. This can be done, for example, by application of the correlation procedure to the reference laser. Then, as illustrated in Fig. 1B, the beat of the reference laser with this comb order is monitored for real time measurement of during operation of the MSS. In the current system the reference laser is stabilized using an internal molecular reference.

The counter-propagating solitons are generated in a high- silica microresonator with 3 mm diameter and corresponding 22 GHz soliton repetition rate lee2012chemically (). Details of the soliton generation process can be found elsewhere yi2015soliton (); yi2016active (); yang2017counter (). Typical optical spectra of cw and ccw solitons are plotted in Fig. 1E and span the telecommunication C-band. The distinct pumping frequencies enable repetition rate tuning to control through the Raman self-frequency shift milian2015solitons (); karpov2016raman (); yi2016theory (); yang2016spatial (); yang2017counter (). For example, a repetition rate difference of kHz as seen in Fig. 1D results from a pumping frequency difference of MHz ().

As a preliminary test, the frequency of an external-cavity-diode-laser is measured and compared against a wavemeter. Fig. 1C and 1D () are from this measurement. The real-time measured wavelength of the laser is presented in Fig. 1F and fluctuates within pm over a 5 ms time interval. The measurement is repeated from 1545 to 1560 nm and the acquired wavelengths are plotted in Fig. 1G. The data show residual deviations less than 0.1 pm versus a wavemeter measurement, which is believed to be limited primarily by the wavemeter resolution ( pm). The systematic uncertainty of the absolute wavelength measurement in the current setup is around MHz ( pm) and is dominated by stability of the reference laser.

The large, microwave-rate, free-spectral range of the MSS enables tracking of fast-chirping lasers in real time and discontinuous broadband tuning. Although correlation is performed with a time interval , the instantaneous frequency of the laser relative to the combs can be acquired at a much faster rate set by the desired time-bandwidth-limited resolution. To avoid aliasing of correlation measurement (i.e., to determine uniquely), the amount of frequency-chirping should not exceed the repetition rate within the measurement window , which imposes a maximum resolvable chirping-rate of . This theoretical limit is 1 PHz/s for the MSS and represents a boost of compared with previous Vernier spectrometers giorgetta2010fast ().

To test the MSS dynamically, it is first used to measure rapid continuous-tuning of an external cavity diode laser. As shown in the upper panel of Fig. 2A, the correlation measurement evolves as the laser is tuned over multiple FSRs of the comb and thereby determines the index as a function of time. The frequency of the scanning laser is displayed at low resolution in the middle panel of Fig. 2A and shows a linear chirping-rate of THz/s. Finally, the lower panel in Fig. 2A shows the measured frequency versus time at higher resolution by removing the average linear frequency ramp. As discussed in the Methods Section, the discontinuities in the measurement are caused by electrical frequency dividers used to reduce the detected signal frequency for processing by a low-bandwidth oscilloscope. These dividers can be eliminated by using a faster oscilloscope. In Fig. 2B the MSS is used to resolve broadband step tuning (mode hopping) of an integrated ring resonator based tunable III-V/Silicon laser diode Tran2018 (). Fast step tuning between 1551.427 nm and 1557.613 nm every 1 ms with the corresponding index stepping between and is observed. The lower panel in Fig. 2B gives a higher resolution zoom-in of one of the step regions. The data points in these measurements are each acquired over 1s so the resolution is approximately 1 MHz.

This combination of speed and precision is also useful for spectroscopic measurements of gas-phase chemicals using tunable, single-frequency lasers. Figure 2C is an absorption line of HCN at 5 Torr obtained by a scanning laser calibrated by the MSS. The linewidth is around 2.6 GHz and the absorbance is as weak as 0.12 dB. Separate measurements on vibronic transitions between the ground state and 2 states were performed. Fig. 2D summarizes the corresponding pseudo-Voigt fitting for the transition wavenumbers, which are in excellent agreement with the HITRAN database gordon2017hitran2016 ().

To illustrate a measurement of more complex multi-line spectra, a fiber mode-locked laser (FMLL) is characterized as shown in Fig. 3A. For this measurement, the FMLL was first sent through a bandpass filter to prevent detector saturation. Also, the frequency extraction procedure differs and is modified to enable unique identification of many frequencies (see Supplement). The FMLL line spacing of 249.7 MHz (measured by photodetection) is not resolved in the Fig. 3B spectrum measured using a grating spectrometer. On the other hand, the reconstructed FMLL spectrum measured using the MSS is plotted in Fig. 3C; here, the comb lines are resolved and their frequency separations closely match the value measured by photo detection. Further details on this measurement are provided in the Supplemental section. In a second study of the FMLL, the MSS is used to measure 6 closely-spaced-in-frequency groups of lines located at various spectral locations spanning 2500 free-spectral-range’s of the mode locked laser. The measured frequencies are plotted in Fig. 3D. A linear fitting defined as is plotted for comparison by using the measured FMLL repetition rate MHz where and represents the relative comb index and fitted offset frequency at , respectively. The residual deviation between the measurement and linear fitting is shown in Fig. 3E and gives excellent agreement. The slight tilt observed in Fig. 3E is believed to be related to drifting of soliton repetition rates which were not monitored real-time. Also, variance of residuals within each group comes from the 300 kHz linewidth of each FMLL line. Drifting of the reference laser and FMLL carrier-envelope offset also contributes to the observed residuals across different measurements.

In conclusion, a soliton spectrometer has been demonstrated using dual-locked counter-propagating soliton microcombs. The device provides high resolution measurement of rapid continuously and step tuned lasers as well as complex multi-line spectra. In combination with a tunable laser, precise measurement of absorption spectra including random spectral access (as opposed to only continuous spectral scanning) can be performed. Further optimization of this system could include generation of solitons from distinct mode families thereby allowing tens-of-MegaHertz repetition rate offset to be possible lucas2018spatial (). If such solitons can be dual-locked, the increased acquisition speed would enable measurement of chirping-rates close to 1 EHz/s. Operation beyond the telecommunications band would also clearly be useful and could employ soliton broadening either internally brasch2016photonic () or using on-chip broadeners lamb2018optical (). Besides the performance enhancement realized with the soliton microcombs, the use of dual-locked counter-propagating solitons provides a considerable technical simplification by eliminating the need for a second mutually phase locked comb. Also, it is interesting to note that the counter-propagating dual-locked solitons are potentially useful in a different application wherein dual-comb down conversion is used to perform TeraHertz spectroscopy kliebisch2018unambiguous (). Finally, chip integrable versions of the current device employing silicon nitride waveguides are possible yang2018bridging (). These and other recently demonstrated compact and low-power soliton systems stern2018battery (); liu2018ultralow () point towards the possibility of compact microresonator soliton spectrometers.


Experimental details. The bandwidth limit of the oscilloscope used in this experiment is 2.5 GHz and in order to measure frequencies up to 11 GHz, microwave frequency dividers were used that function between 0.5 GHz to 10 GHz and provide an 8 division ratio. The use of these dividers created 3 GHz frequency unresolvable bands within one FSR of the optical combs, which caused the discontinuities in the lower panel in Fig. 2A. Meanwhile, the repetition rate difference corresponding to the divided signals will also decrease proportionally by a factor of 8, which in turn reduces the maximum resolvable chirping rate to 125 THz/s. The dividers can be omitted by using a higher-bandwidth oscilloscope, which eliminates the above unresolvable bands and allows chirp-rate measurements approaching the theoretical limit.

The pump is a fiber laser with free-running linewidth less than 2 kHz over 100 ms Lee2014spiral (). The long term stability of the soliton is maintained by introducing a feed back loop control yi2015soliton (); yi2016active ().


The authors gratefully acknowledge the Defense Advanced Research Projects Agency (DARPA) under the SCOUT (W911NF-16-1-0548) and DODOS (HR0011-15-C-055) programs; the Air Force Office of Scientific Research (FA9550-18-1-0353) and the Kavli Nanoscience Institute.


  • (1) Willner, A., Yu, C. & Pan, Z. Optical Fiber Telecommunications VB (Fifth Edition): Chapter 7 (Academic Press, 2008).
  • (2) Allen, M. G. Diode laser absorption sensors for gas-dynamic and combustion flows. Meas. Sci. Technol. 9, 545 (1998).
  • (3) Choma, M. A., Sarunic, M. V., Yang, C. & Izatt, J. A. Sensitivity advantage of swept source and fourier domain optical coherence tomography. Opt. Express 11, 2183–2189 (2003).
  • (4) Jones, D. J. et al. Carrier-envelope phase control of femtosecond mode-locked lasers and direct optical frequency synthesis. Science 288, 635–639 (2000).
  • (5) Holzwarth, R. et al. Optical frequency synthesizer for precision spectroscopy. Phys. Rev. Lett. 85, 2264 (2000).
  • (6) Diddams, S. A. The evolving optical frequency comb. J. Opt. Soc. Am. B 27, B51–B62 (2010).
  • (7) Del’Haye, P., Arcizet, O., Gorodetsky, M. L., Holzwarth, R. & Kippenberg, T. J. Frequency comb assisted diode laser spectroscopy for measurement of microcavity dispersion. Nat. Photon. 3, 529 (2009).
  • (8) Coddington, I., Giorgetta, F. R., Baumann, E., Swann, W. C. & Newbury, N. R. Characterizing fast arbitrary cw waveforms with 1500 thz/s instantaneous chirps. IEEE J. Sel. Top. Quantum Electron. 18, 228–238 (2012).
  • (9) Giorgetta, F., Coddington, I., Baumann, E., Swann, W. & Newbury, N. Fast high-resolution spectroscopy of dynamic continuous-wave laser sources. Nat. Photon. 4, 853 (2010).
  • (10) Ma, L.-S., Zucco, M., Picard, S., Robertsson, L. & Windeler, R. S. A new method to determine the absolute mode number of a mode-locked femtosecond-laser comb used for absolute optical frequency measurements. IEEE J. Sel. Top. Quantum Electron. 9, 1066–1071 (2003).
  • (11) Peng, J.-L., Liu, T.-A. & Shu, R.-H. Optical frequency counter based on two mode-locked fiber laser combs. Appl. Phys. B 92, 513–518 (2008).
  • (12) Coddington, I., Newbury, N. & Swann, W. Dual-comb spectroscopy. Optica 3, 414–426 (2016).
  • (13) Suh, M.-G., Yang, Q.-F., Yang, K. Y., Yi, X. & Vahala, K. J. Microresonator soliton dual-comb spectroscopy. Science 354, 600–603 (2016).
  • (14) Yang, Q.-F., Yi, X., Yang, K. Y. & Vahala, K. Counter-propagating solitons in microresonators. Nat. Photon. 11, 560–564 (2017).
  • (15) Kippenberg, T. J., Gaeta, A. L., Lipson, M. & Gorodetsky, M. L. Dissipative kerr solitons in optical microresonators. Science 361 (2018).
  • (16) Herr, T. et al. Temporal solitons in optical microresonators. Nat. Photon. 8, 145–152 (2014).
  • (17) Yi, X., Yang, Q.-F., Yang, K. Y., Suh, M.-G. & Vahala, K. Soliton frequency comb at microwave rates in a high-q silica microresonator. Optica 2, 1078–1085 (2015).
  • (18) Brasch, V. et al. Photonic chip–based optical frequency comb using soliton cherenkov radiation. Science 351, 357–360 (2016).
  • (19) Wang, P.-H. et al. Intracavity characterization of micro-comb generation in the single-soliton regime. Opt. Express 24, 10890–10897 (2016).
  • (20) Joshi, C. et al. Thermally controlled comb generation and soliton modelocking in microresonators. Opt. Lett. 41, 2565–2568 (2016).
  • (21) Gong, Z. et al. High-fidelity cavity soliton generation in crystalline aln micro-ring resonators. Opt. Lett. 43, 4366–4369 (2018).
  • (22) Lee, H. et al. Chemically etched ultrahigh-q wedge-resonator on a silicon chip. Nat. Photon. 6, 369–373 (2012).
  • (23) Yi, X., Yang, Q.-F., Youl, K. & Vahala, K. Active capture and stabilization of temporal solitons in microresonators. Opt. Lett. 41, 2037–2040 (2016).
  • (24) Milián, C., Gorbach, A. V., Taki, M., Yulin, A. V. & Skryabin, D. V. Solitons and frequency combs in silica microring resonators: Interplay of the raman and higher-order dispersion effects. Phys. Rev. A 92, 033851 (2015).
  • (25) Karpov, M. et al. Raman self-frequency shift of dissipative kerr solitons in an optical microresonator. Phys. Rev. Lett. 116, 103902 (2016).
  • (26) Yi, X., Yang, Q.-F., Yang, K. Y. & Vahala, K. Theory and measurement of the soliton self-frequency shift and efficiency in optical microcavities. Opt. Lett. 41, 3419–3422 (2016).
  • (27) Yang, Q.-F., Yi, X., Yang, K. Y. & Vahala, K. Spatial-mode-interaction-induced dispersive-waves and their active tuning in microresonators. Optica 3, 1132–1135 (2016).
  • (28) Tran, M. A., Huang, D., Komljenovic, T., Peters, J. & Bowers, J. E. A 2.5 khz linewidth widely tunable laser with booster soa integrated on silicon. Proceedings of the 2018 IEEE International Semiconductor Laser Conference, Santa Fe 1–2 (2018).
  • (29) Gordon, I. E. et al. The HITRAN2016 molecular spectroscopic database. J. Quant. Spectrosc. Radiat. Transf. 203, 3–69 (2017).
  • (30) Lucas, E. et al. Spatial multiplexing of soliton microcombs. Nat. Photon. 12, 699–705 (2018).
  • (31) Lamb, E. S. et al. Optical-frequency measurements with a kerr microcomb and photonic-chip supercontinuum. Phys. Rev. Applied 9, 024030 (2018).
  • (32) Kliebisch, O. et al. Unambiguous real-time terahertz frequency metrology using dual 10 ghz femtosecond frequency combs. Optica 5, 1431–1437 (2018).
  • (33) Yang, K. Y. et al. Bridging ultrahigh-Q devices and photonic circuits. Nat. Photon. 12, 297 (2018).
  • (34) Stern, B., Ji, X., Okawachi, Y., Gaeta, A. L. & Lipson, M. Battery-operated integrated frequency comb generator. Nature 562, 401 (2018).
  • (35) Liu, J. et al. Ultralow-power chip-based soliton microcombs for photonic integration. Optica 5, 1347–1353 (2018).
  • (36) Lee, H. et al. Spiral resonators for on-chip laser frequency stabilization. Nat. Commun. 4, 2468 (2013).
Comments 0
Request Comment
You are adding the first comment!
How to quickly get a good reply:
  • Give credit where it’s due by listing out the positive aspects of a paper before getting into which changes should be made.
  • Be specific in your critique, and provide supporting evidence with appropriate references to substantiate general statements.
  • Your comment should inspire ideas to flow and help the author improves the paper.

The better we are at sharing our knowledge with each other, the faster we move forward.
The feedback must be of minimum 40 characters and the title a minimum of 5 characters
Add comment
Loading ...
This is a comment super asjknd jkasnjk adsnkj
The feedback must be of minumum 40 characters
The feedback must be of minumum 40 characters

You are asking your first question!
How to quickly get a good answer:
  • Keep your question short and to the point
  • Check for grammar or spelling errors.
  • Phrase it like a question
Test description