Pith. sign in

REVIEW 3 major objections 5 minor 52 references

Dual-Frequency Comb in Fiber Fabry-Perot Resonator

T0 review · 3 major / 5 minor · reviewed 2026-08-08 · deepseek-v4-flash

Pith's one-line read A single fiber Fabry-Perot cavity generates two mutually coherent optical frequency combs, one per polarization mode, with repetition rates differing by 6 kHz.

desk verdict Solid first demonstration of dual-comb generation in a passive fiber Fabry-Perot cavity; the coherence evidence is adequate but not airtight. read the letter →

arxiv 2502.07392 v1 pith:ZC5NZTCB submitted 2025-02-11 physics.optics

classification physics.optics PACS 42.60.Da42.62.Fi42.65.Ky
keywords dual-combspectroscopyfiberFabry-PerotresonatorswitchingwavesopticalfrequencycombbirefringenceKerrnormaldispersion
verification ladder T0 review T1 audit T2 compute T3 formal

The pith

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The reading

The paper claims to demonstrate the first dual-comb source built from a single passive fiber Fabry-Perot resonator. By pumping the two orthogonal polarization modes of the same cavity with pulse trains at slightly different repetition rates, two switching-wave-induced optical frequency combs are generated, each spanning roughly 40 nm and differing in line spacing by 6 kHz. Recombining the two combs produces a dual-comb interferogram whose 6 kHz beatnote carries the optical spectrum down-converted to the radio-frequency domain. The authors prove the concept by measuring a programmable filter's transfer function at 1.696 GHz resolution in 7 ms, a speed and resolution combination that ordinary optical spectrum analyzers do not reach. The significance is that a single compact, fiber-integrated cavity can supply both arms of a dual-comb spectrometer with mutual coherence inherited from a common pump laser.

What carries the argument

The load-bearing mechanism is switching waves, which are steep fronts connecting two homogeneous states in a normal-dispersion, bistable cavity; these are excited by short pulses and broaden the spectrum into a Kerr comb. The cavity's residual birefringence splits its resonances into two polarization families with free spectral ranges differing by 6 kHz, so a single resonator holds two distinct comb spacings. Two synchronously pumped pulse trains, offset in frequency to match the mode families, excite each comb independently, while a single Pound-Drever-Hall-style lock on one mode's nonlinear signal stabilizes both. The free spectral range difference, and thus the dual-comb beat frequency, can be tuned by mechanically stressing the fiber to change its birefringence.

What would settle it

Send the two pumps into the cavity with one comb temporarily blocked, and measure the residual light in the blocked polarization channel as a function of pump power; if the extinction ratio worsens beyond the polarization beam splitter's 20 dB spec when the pump of the other mode is strong, intra-cavity cross-talk is present. Alternatively, measure the mutual coherence of the 6 kHz beatnote when the cavity is mechanically stressed to change birefringence; a sudden increase in linewidth or a floor in the Allan deviation would indicate that the two combs are not fully independent.

Watch

Extended reading notes

Core claim

The central discovery is that the birefringence of a normal-dispersion fiber Fabry-Perot resonator provides two polarization modes with slightly different free spectral ranges (1.696 GHz and 1.696 GHz + 6 kHz), and both modes can be driven into switching-wave Kerr comb states simultaneously by two phase-coherent pulsed pumps derived from a single laser. The resulting orthogonally polarized combs are mutually coherent, have narrow beatnotes (less than 15 Hz linewidth), and remain stable across their 40 nm bandwidth, with phase noise and Allan deviation matching the driving electronics. Combining the combs yields an RF interferogram with a 6 kHz repetition rate, and the retrieved spectra resolve teeth spaced by the cavity FSR of 1.696 GHz, something a 12 GHz-resolution OSA cannot do, in 7 ms. This is, to the authors' knowledge, the first dual-comb source in a passive fiber Fabry-Perot cavity.

Load-bearing premise

The claim that the two combs are mutually coherent and independent rests on the assumption that the two polarization modes do not interact nonlinearly inside the shared 6 cm fiber; the paper infers this from the extinction ratio of the output polarizing beam splitter rather than from a direct measurement of intra-cavity coupling.

Editorial extensions

If this is right

  • Dual-comb spectroscopy at the cavity free-spectral-range resolution (1.696 GHz) can be performed in 7 ms with a single fiber cavity and simple electronics, compared to seconds with an optical spectrum analyzer.
  • The repetition-rate difference is set by the cavity birefringence and can be tuned by mechanical stress, offering a direct dial for acquisition speed versus RF-comb span.
  • Because both combs are derived from a single laser and cavity, the mutual coherence is inherited from the common source, avoiding the need for separate stabilization loops.
  • Resolution and acquisition time can be further adjusted by changing the cavity length or by using rational harmonic driving to increase effective line spacing.

Reading between the lines

Editorial extensions of the paper, not claims the author makes directly.

  • If the mutual coherence survives higher pump powers, the same cavity could serve dual-comb ranging or imaging, where the 6 kHz comb spacing defines a 166-microsecond update rate.
  • A direct measurement of intra-cavity polarization coupling, rather than relying on the PBS extinction ratio, would sharpen the claim of independence, and an improved polarizer or in-fiber mode filter might push the extinction beyond 40 dB.
  • The switching-wave mechanism is not specific to fiber; the same polarization-multiplexing scheme could be transferred to normal-dispersion microresonators to create compact dual-comb sources on a chip.
  • Locking the 6 kHz beatnote to an external RF reference could reduce the measured white-frequency-noise floor, making the source suitable for longer integration in spectroscopy.
Share X Bluesky LinkedIn Reddit HN

Signed reviews

No signed human review yet.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, and a circularity audit.

Referee Report

3 major / 5 minor

Summary. The manuscript reports an experimental demonstration of a dual-frequency comb source based on switching-wave generation in a single passive fiber Fabry-Perot resonator. Two orthogonally polarized modes of the cavity, having slightly different free spectral ranges (FSRs) due to fiber birefringence, are pumped by electro-optically generated pulse trains at matched repetition rates. The authors generate two optical combs with 40 nm bandwidth each and a repetition-rate difference of 6 kHz, measure the dual-comb interferogram, and demonstrate a proof-of-concept spectroscopy measurement of a programmable optical filter. The paper claims a spectral resolution equal to the cavity FSR (1.696 GHz) with a 7 ms acquisition time, and positions the result as the first dual-comb source in a passive fiber Fabry-Perot cavity.

Significance. If the central claims hold, this is a meaningful contribution to dual-comb technology. The approach exploits the intrinsic birefringence of a fiber Fabry-Perot cavity to produce two combs from a single pump laser, avoiding two separate resonators or pump lasers and potentially improving mutual coherence. The work builds on the authors' prior switching-wave comb results and includes numerical agreement, stability characterization, and a spectroscopy demonstration. The demonstrated tunability of the line-spacing difference (1-6 kHz) via mechanical stress is also valuable. However, the mutual coherence of the two combs and the claimed resolution are not directly quantified: the 6 kHz dual-comb beat shows 20 dB higher phase noise than the individual comb beat, and the RF comb lines are not shown resolved in a high-resolution spectrum. These points are central to the dual-comb claim, so the core result is defensible but requires additional evidence.

major comments (3)
  1. [Section IV, Fig. 3(a) and Fig. 4(b)-(d)] The paper does not report the linewidth of the individual 6 kHz RF comb lines, nor does it show a high-resolution spectrum with clearly resolved lines separated by 6 kHz; the inset in Fig. 4 is described qualitatively. Since the claimed dual-comb spectroscopy resolution of 1.696 GHz requires that adjacent RF comb lines be individually resolvable, and the 6 kHz beat exhibits 20 dB higher phase noise with spurs at harmonics of 6 kHz, the mutual coherence and resolution claim are not fully supported. Please provide a high-resolution RF spectrum (e.g., with resolution bandwidth much smaller than 6 kHz) showing resolved comb lines and their linewidths.
  2. [Section III, cross-talk paragraph] The independence of the two polarization modes is inferred from a single-pump measurement and attributed to PBS extinction rather than intra-cavity coupling, based on the statement "suggesting that this component is the main cause of cross-talk rather than signal mixing within the cavity itself." This is not a direct measurement. Under dual-pump operation at 500 mW peak power in a highly nonlinear fiber (γ = 10.8 W⁻¹km⁻¹, L = 6.07 cm), nonlinear polarization coupling could degrade mutual coherence. Please measure the cross-talk or mode coupling under dual-pump conditions, or provide a quantitative estimate of the expected intra-cavity nonlinear coupling.
  3. [Section V, Fig. 5] The proof-of-concept spectroscopy uses a notch filter with 25 GHz FWHM, which is much broader than the claimed 1.696 GHz resolution. Agreement between the dual-comb and OSA measurements of this broad feature cannot validate that individual comb teeth are resolved. To support the resolution claim, the measurement should be repeated with a spectral feature narrower than the FSR, or the resolved RF comb lines should be directly demonstrated.
minor comments (5)
  1. [Abstract and Section V] The word "monolitic" should be "monolithic" in both places.
  2. [Section IV, paragraph after Eq. (1)] The sentence "being the the optical frequency span" contains a duplicated "the".
  3. [Fig. 2(e)] The colormap lacks a colorbar and axis labels; the text refers to a "colormap" but it is not clear what quantity is plotted as a function of frequency shift and filter position.
  4. [Section II, f0 notation] The symbol f0 is used both for the polarization-mode offset (643 MHz) and for the center frequency of the RF spectrum in Section IV; please clarify the notation to avoid ambiguity.
  5. [Section III, simulation comparison] The simulations are said to be obtained from an extended Lugiato-Lefever equation, but the specific parameter values (detuning, pump power, coupling) used for the numerical curves in Fig. 2 are not given; providing them would improve reproducibility.

Circularity Check

0 steps flagged · score 0.0 of 10

No significant circularity: the paper is an experimental demonstration; the 6 kHz spacing is a set operating point from the synthesizers and measured FSR difference, not a fitted parameter relabeled as a prediction.

full rationale

The central claim is an experimental result, not a derivation from first principles. The FSR values (FSRs ≈ 1.696 GHz, FSRp = FSRs + 6 kHz) are independently measured, and the pump repetition rates are then deliberately set to match these cavity roundtrips; the equality ∆f = FSRp − FSRs = frep.p − frep.s = 6 kHz is therefore a statement of the intended operating condition, not a prediction extracted from the interferogram. The comb simulations are obtained from the Lugiato-Lefever equation with stated physical parameters and are compared to the measured spectra, so this is an independent numerical check rather than a self-definitional loop. The stability claims are supported by direct phase-noise and Allan-deviation measurements, even though some supporting citations are to the authors' prior work; those citations are supplemented by in-paper data and do not carry the argument alone. The cross-talk attribution to the PBS is an inference, but inferences or measurement limitations are not circularity. The only 'by construction' relation is the pump-imposed repetition-rate difference, and the paper never presents that relation as a derived physical prediction, so no fitted input is renamed as a prediction. Concerns about RF comb linewidth or mutual coherence are evidence-quality issues outside the circularity axis.

Assumptions & free parameters 1 free parameters · 5 assumptions · 0 invented entities

The central claim is an experimental demonstration; no numerical result is obtained by fitting parameters to data. The listed axiom entries are the background physical models and the polarization-independence assumption the demonstration relies on. No invented entities are introduced.

free parameters (1)
  • Pump-cavity detuning setpoint delta = 0.023 rad
    Chosen manually as the PID setpoint that yields symmetric switching-wave combs (Section III). This is a control parameter of the demonstration, not fitted to a target.
assumptions (5)
  • domain assumption Kerr frequency comb formation in fiber Fabry-Perot resonators is governed by the extended Lugiato-Lefever equation used in refs 28 and 42.
    Invoked in Section III to model the observed combs; background from the authors' prior work and standard cavity theory.
  • domain assumption Pulse pumping at normal dispersion generates switching-wave combs that inherit the pump repetition rate and mutual coherence.
    Assumed from prior studies (refs 28, 29, 38); used to align frep to FSR and to interpret the symmetric comb shoulders.
  • ad hoc to paper The two polarization modes of the cavity are independent and linear, and cross-talk is dominated by the PBS rather than intra-cavity coupling.
    Stated in Section III as a suggestion rather than a direct measurement; supports treating the two combs as independent sources.
  • domain assumption The single-sideband frequency shift fSSB = f0 + 17 FSRp places the p-mode pump at the same detuning as the s-mode pump.
    Assumed in Section II; relies on f0 being constant at the pump wavelength.
  • domain assumption The phase noise of the generated combs follows the driving synthesizer and the common CW laser.
    Based on refs 11, 12, 43; used in Section III to interpret the stability plots.

how reviews work

0 comments
Cite this review

Pith. "Pith review of Dual-Frequency Comb in Fiber Fabry-Perot Resonator." pith.science (2026). https://pith.science/paper/ZC5NZTCB

@misc{pith2026250207392,
  author       = {Pith},
  title        = {Pith review of: Dual-Frequency Comb in Fiber Fabry-Perot Resonator},
  year         = {2026},
  howpublished = {\url{https://pith.science/paper/ZC5NZTCB}},
  note         = {Machine review of arXiv:2502.07392}
}
read the original abstract

This paper presents a novel approach to dual-frequency comb generation utilizing a single fiber Fabry-Perot resonator, advancing the implementation of these sources in fiber-based systems. Dual-comb applications such as spectroscopy, ranging, and imaging, known for their high-resolution and rapid data acquisition capabilities, benefit significantly from the stability and coherence of optical frequency comb sources. Our method leverages the birefringent property of the resonator induced by the optical fiber to generate two orthogonally polarized optical frequency combs in a monolitic resonator. This approach allows for the generation of two different frequency combs with slightly different repetition rates, exhibiting excellent mutual coherence, making it highly relevant for dual-comb applications. The 40 nm bandwidth generated combs are induced by switching-waves in a normal dispersion fiber Fabry-Perot resonator. These comb types have the advantage of being easily generated by a pulse pumping scheme, which is employed in this study. Finally, the potential of the source is demonstrated by a proof-of-concept spectroscopy measurement.

Figures

Figures reproduced from arXiv: 2502.07392 by the authors.

Figure 1
Figure 1. FIG. 1. Experimental setup. (a) Representation of the resonance [PITH_FULL_IMAGE:figures/full_fig_p002_1.png] view at source ↗
Figure 2
Figure 2. FIG. 2. Optical frequency combs in both polarization mode. (a) Measurement on the polarization mode [PITH_FULL_IMAGE:figures/full_fig_p003_2.png] view at source ↗
Figure 3
Figure 3. FIG. 3. Frequency stability. (a) Phase noise spectra; (b) Allan deviation. The legend in (a) applies to both boxes and includes the central [PITH_FULL_IMAGE:figures/full_fig_p004_3.png] view at source ↗
Figures from the paper (2 more)
Figure 4
Figure 4. Figure 4: FIG. 4. Dual-comb source measurement in the RF domain. (a) Multi [PITH_FULL_IMAGE:figures/full_fig_p005_4.png]
Figure 5
Figure 5. Figure 5: FIG. 5. Proof-of-concept spectroscopic measurement. (a) Three RF combs; red lines: the pulsed pump, blue lines: the generated comb, green [PITH_FULL_IMAGE:figures/full_fig_p006_5.png]

Discussion (0). Continue with ORCID to comment.

Reference graph

Works this paper leans on

52 extracted references · 5 canonical work pages

  1. [1]

    merlin.mbs aapmrev4-1.bst 2010-07-25 4.21a (PWD, AO, DPC) hacked

    FUNCTION id.bst "merlin.mbs aapmrev4-1.bst 2010-07-25 4.21a (PWD, AO, DPC) hacked" ENTRY address archive archivePrefix author bookaddress booktitle chapter collaboration doi edition editor eid eprint howpublished institution isbn issn journal key language month note number organization pages primaryClass publisher school SLACcitation series title translat...

  2. [2]

    merlin.mbs aipauth4-1.bst 2010-07-25 4.21a (PWD, AO, DPC) hacked

    FUNCTION id.bst "merlin.mbs aipauth4-1.bst 2010-07-25 4.21a (PWD, AO, DPC) hacked" ENTRY address archive archivePrefix author bookaddress booktitle chapter collaboration doi edition editor eid eprint howpublished institution isbn issn journal key language month note number organization pages primaryClass publisher school SLACcitation series title translat...

  3. [3]

    merlin.mbs aipnum4-1.bst 2010-07-25 4.21a (PWD, AO, DPC) hacked

    FUNCTION id.bst "merlin.mbs aipnum4-1.bst 2010-07-25 4.21a (PWD, AO, DPC) hacked" ENTRY address archive archivePrefix author bookaddress booktitle chapter collaboration doi edition editor eid eprint howpublished institution isbn issn journal key language month note number organization pages primaryClass publisher school SLACcitation series title translati...

  4. [4]

    merlin.mbs apsrev4-1.bst 2010-07-25 4.21a (PWD, AO, DPC) hacked

    FUNCTION id.bst "merlin.mbs apsrev4-1.bst 2010-07-25 4.21a (PWD, AO, DPC) hacked" ENTRY address archive archivePrefix author bookaddress booktitle chapter collaboration doi edition editor eid eprint howpublished institution isbn issn journal key language month note number organization pages primaryClass publisher school SLACcitation series title translati...

  5. [5]

    merlin.mbs apsrmp4-1.bst 2010-07-25 4.21a (PWD, AO, DPC) hacked

    FUNCTION id.bst "merlin.mbs apsrmp4-1.bst 2010-07-25 4.21a (PWD, AO, DPC) hacked" ENTRY address archive archivePrefix author bookaddress booktitle chapter collaboration doi edition editor eid eprint howpublished institution isbn issn journal key language month note number organization pages primaryClass publisher school SLACcitation series title translati...

  6. [6]

    Fortier \ and\ author E

    author author T. Fortier \ and\ author E. Baumann ,\ title title 20 years of developments in optical frequency comb technology and applications , \ 10.1038/s42005-019-0249-y journal journal Communications Physics \ volume 2 ,\ pages 153 ( year 2019 ) NoStop

  7. [7]

    Torres-Company \ and\ author A

    author author V. Torres-Company \ and\ author A. M. \ Weiner ,\ title title Optical frequency comb technology for ultra-broadband radio-frequency photonics: Optical frequency comb technology for RF photonics , \ 10.1002/lpor.201300126 journal journal Laser & Photonics Reviews \ volume 8 ,\ pages 368--393 ( year 2014 ) NoStop

  8. [8]

    Picqué \ and\ author T

    author author N. Picqué \ and\ author T. W. \ Hänsch ,\ title title Frequency comb spectroscopy , \ 10.1038/s41566-018-0347-5 journal journal Nature Photonics \ volume 13 ,\ pages 146--157 ( year 2019 ) NoStop

Show all 52 references
  1. [9]

    author author S. A. \ Diddams , author L. Hollberg , \ and\ author V. Mbele ,\ title title Molecular fingerprinting with the resolved modes of a femtosecond laser frequency comb , \ 10.1038/nature05524 journal journal Nature \ volume 445 ,\ pages 627--630 ( year 2007 ) NoStop

  2. [10]

    Mandon , author G

    author author J. Mandon , author G. Guelachvili , \ and\ author N. Picqué ,\ title title Fourier transform spectroscopy with a laser frequency comb , \ 10.1038/nphoton.2008.293 journal journal Nature Photonics \ volume 3 ,\ pages 99--102 ( year 2009 ) NoStop

  3. [11]

    Coddington , author N

    author author I. Coddington , author N. Newbury , \ and\ author W. Swann ,\ title title Dual-comb spectroscopy , \ 10.1364/OPTICA.3.000414 journal journal Optica \ volume 3 ,\ pages 414 ( year 2016 ) NoStop

  4. [12]

    author author S. M. \ Link , author A. Klenner , author M. Mangold , author C. A. \ Zaugg , author M. Golling , author B. W. \ Tilma , \ and\ author U. Keller ,\ title title Dual-comb modelocked laser , \ 10.1364/OE.23.005521 journal journal Optics Express \ volume 23 ,\ pages...

  5. [13]

    Ideguchi , author T

    author author T. Ideguchi , author T. Nakamura , author Y. Kobayashi , \ and\ author K. Goda ,\ title title Kerr-lens mode-locked bidirectional dual-comb ring laser for broadband dual-comb spectroscopy , \ 10.1364/OPTICA.3.000748 journal journal Optica \ volume 3 ,\ pages 748 ...

  6. [14]

    Li , author J

    author author B. Li , author J. Xing , author D. Kwon , author Y. Xie , author N. Prakash , author J. Kim , \ and\ author S.-W. \ Huang ,\ title title Bidirectional mode-locked all-normal dispersion fiber laser , \ 10.1364/OPTICA.396304 journal journal Optica \ volume 7 ,\ pag...

  7. [15]

    Mehravar , author R

    author author S. Mehravar , author R. A. \ Norwood , author N. Peyghambarian , \ and\ author K. Kieu ,\ title title Real-time dual-comb spectroscopy with a free-running bidirectionally mode-locked fiber laser , \ 10.1063/1.4953400 journal journal Applied Physics Letters \ volu...

  8. [16]

    \ Bancel , author E

    author author E.-L. \ Bancel , author E. Genier , author R. Santagata , author M. Conforti , author A. Kudlinski , author G. Bouwmans , author O. Vanvcincq , author D. Labat , author A. Cassez , \ and\ author A. Mussot ,\ title title All-fiber frequency agile triple-frequency ...

  9. [17]

    Parriaux , author K

    author author A. Parriaux , author K. Hammani , \ and\ author G. Millot ,\ title title Electro-optic frequency combs , \ 10.1364/AOP.382052 journal journal Advances in Optics and Photonics \ volume 12 ,\ pages 223 ( year 2020 ) NoStop

  10. [18]

    Bao , author M.-G

    author author C. Bao , author M.-G. \ Suh , \ and\ author K. Vahala ,\ title title Microresonator soliton dual-comb imaging , \ 10.1364/OPTICA.6.001110 journal journal Optica \ volume 6 ,\ pages 1110 ( year 2019 ) NoStop

  11. [19]

    Dutt , author C

    author author A. Dutt , author C. Joshi , author X. Ji , author J. Cardenas , author Y. Okawachi , author K. Luke , author A. L. \ Gaeta , \ and\ author M. Lipson ,\ title title On-chip dual-comb source for spectroscopy , \ 10.1126/sciadv.1701858 journal journal Science Advanc...

  12. [20]

    \ Suh , author Q.-F

    author author M.-G. \ Suh , author Q.-F. \ Yang , author K. Y. \ Yang , author X. Yi , \ and\ author K. J. \ Vahala ,\ title title Microresonator soliton dual-comb spectroscopy , \ 10.1126/science.aah6516 journal journal Science \ volume 354 ,\ pages 600--603 ( year 2016 ) NoStop

  13. [21]

    Trocha , author M

    author author P. Trocha , author M. Karpov , author D. Ganin , author M. H. P. \ Pfeiffer , author A. Kordts , author S. Wolf , author J. Krockenberger , author P. Marin-Palomo , author C. Weimann , author S. Randel , author W. Freude , author T. J. \ Kippenberg , \ and\ autho...

  14. [22]

    Rebolledo-Salgado , author C

    author author I. Rebolledo-Salgado , author C. Quevedo-Galán , author O. B. \ Helgason , author A. Lööf , author Z. Ye , author F. Lei , author J. Schroder , author M. Zelan , \ and\ author V. Torres-Company ,\ title title Platicon dynamics in photonic molecules , \ 10.1038/s4...

  15. [23]

    Sun , author J

    author author Y. Sun , author J. Wu , author M. Tan , author X. Xu , author Y. Li , author R. Morandotti , author A. Mitchell , \ and\ author D. J. \ Moss ,\ title title Applications of optical microcombs , \ 10.1364/AOP.470264 journal journal Advances in Optics and Photonics ...

  16. [24]

    \ Suh \ and\ author K

    author author M.-G. \ Suh \ and\ author K. J. \ Vahala ,\ title title Soliton microcomb range measurement , \ 10.1126/science.aao1968 journal journal Science \ volume 359 ,\ pages 884--887 ( year 2018 ) NoStop

  17. [25]

    Zhang , author T

    author author H. Zhang , author T. Tan , author H.-J. \ Chen , author Y. Yu , author W. Wang , author B. Chang , author Y. Liang , author Y. Guo , author H. Zhou , author H. Xia , author Q. Gong , author C. W. \ Wong , author Y. Rao , author Y.-F. \ Xiao , \ and\ author B. Yao...

  18. [26]

    Lucas , author G

    author author E. Lucas , author G. Lihachev , author R. Bouchand , author N. G. \ Pavlov , author A. S. \ Raja , author M. Karpov , author M. L. \ Gorodetsky , \ and\ author T. J. \ Kippenberg ,\ title title Spatial multiplexing of soliton microcombs , \ 10.1038/s41566-018-025...

  19. [27]

    Xu , author M

    author author Y. Xu , author M. Erkintalo , author Y. Lin , author S. Coen , author H. Ma , \ and\ author S. G. \ Murdoch ,\ title title Dual-microcomb generation in a synchronously driven waveguide ring resonator , \ 10.1364/OL.443153 journal journal Optics Letters \ volume 4...

  20. [28]

    Bunel , author M

    author author T. Bunel , author M. Conforti , author Z. Ziani , author J. Lumeau , author A. Moreau , author A. Fernandez , author O. Llopis , author G. Bourcier , \ and\ author A. Mussot ,\ title title 28 THz soliton frequency comb in a continuous-wave pumped fiber Fabry – Pé...

  21. [29]

    Nie , author K

    author author M. Nie , author K. Jia , author Y. Xie , author S. Zhu , author Z. Xie , \ and\ author S.-W. \ Huang ,\ title title Synthesized spatiotemporal mode-locking and photonic flywheel in multimode mesoresonators , \ 10.1038/s41467-022-34103-0 journal journal Nat Commun...

  22. [30]

    Jia , author X

    author author K. Jia , author X. Wang , author D. Kwon , author J. Wang , author E. Tsao , author H. Liu , author X. Ni , author J. Guo , author M. Yang , author X. Jiang , author J. Kim , author S.-n. \ Zhu , author Z. Xie , \ and\ author S.-W. \ Huang ,\ title title Photonic...

  23. [31]

    Obrzud , author S

    author author E. Obrzud , author S. Lecomte , \ and\ author T. Herr ,\ title title Temporal solitons in microresonators driven by optical pulses , \ 10.1038/nphoton.2017.140 journal journal Nature Photonics \ volume 11 ,\ pages 600--607 ( year 2017 ) NoStop

  24. [32]

    Li , author Y

    author author Z. Li , author Y. Xu , author S. Shamailov , author X. Wen , author W. Wang , author X. Wei , author Z. Yang , author S. Coen , author S. G. \ Murdoch , \ and\ author M. Erkintalo ,\ title title Ultrashort dissipative Raman solitons in Kerr resonators driven with...

  25. [33]

    Bunel ,\ title title Broadband Kerr frequency comb in fiber Fabry - Perot resonators induced by switching waves , \ @noop journal journal PHYSICAL REVIEW A \ ( year 2024 ) NoStop

    author author T. Bunel ,\ title title Broadband Kerr frequency comb in fiber Fabry - Perot resonators induced by switching waves , \ @noop journal journal PHYSICAL REVIEW A \ ( year 2024 ) NoStop

  26. [34]

    Xiao , author K

    author author Z. Xiao , author K. Wu , author H. Zhang , author T. Li , author M. Cai , author Y. Huang , \ and\ author J. Chen ,\ title title Modeling the Kerr Comb of a Pulse Pumped F - P Microresonator With Normal Dispersion , \ 10.1109/JLT.2023.3300191 journal journal Jour...

  27. [35]

    Xiao , author T

    author author Z. Xiao , author T. Li , author M. Cai , author H. Zhang , author Y. Huang , author C. Li , author B. Yao , author K. Wu , \ and\ author J. Chen ,\ title title Near-zero-dispersion soliton and broadband modulational instability Kerr microcombs in anomalous disper...

  28. [36]

    Ding , author G

    author author Z. Ding , author G. Wang , author Y. Xiong , author Y. Chen , \ and\ author F. Xu ,\ title title Single-short-cavity dual-comb fiber laser with over 120 kHz repetition rate difference based on polarization multiplexing , \ 10.1364/OL.501835 journal journal Optics...

  29. [37]

    Zhao , author T

    author author X. Zhao , author T. Li , author Y. Liu , author Q. Li , \ and\ author Z. Zheng ,\ title title Polarization-multiplexed, dual-comb all-fiber mode-locked laser , \ 10.1364/PRJ.6.000853 journal journal Photonics Research \ volume 6 ,\ pages 853 ( year 2018 ) NoStop

  30. [38]

    Zideluns , author F

    author author J. Zideluns , author F. Lemarchand , author D. Arhilger , author H. Hagedorn , \ and\ author J. Lumeau ,\ title title Automated optical monitoring wavelength selection for thin-film filters , \ 10.1364/OE.439033 journal journal Optics Express \ volume 29 ,\ pages...

  31. [39]

    Bunel , author M

    author author T. Bunel , author M. Conforti , author Z. Ziani , author J. Lumeau , author A. Moreau , author A. Fernandez , author O. Llopis , author J. Roul , author A. M. \ Perego , author K. K. Y. \ Wong , \ and\ author A. Mussot ,\ title title Observation of modulation ins...

  32. [40]

    Xue , author M

    author author X. Xue , author M. Qi , \ and\ author A. M. \ Weiner ,\ title title Normal-dispersion microresonator Kerr frequency combs , \ 10.1515/nanoph-2016-0016 journal journal Nanophotonics \ volume 5 ,\ pages 244--262 ( year 2016 ) NoStop

  33. [41]

    Fulop , author M

    author author A. Fulop , author M. Mazur , author A. Lorences-Riesgo , author O. B. \ Helgason , author P.-H. \ Wang , author Y. Xuan , author D. E. \ Leaird , author M. Qi , author P. A. \ Andrekson , author A. M. \ Weiner , \ and\ author V. Torres-Company ,\ title title High...

  34. [42]

    Godey , author I

    author author C. Godey , author I. V. \ Balakireva , author A. Coillet , \ and\ author Y. K. \ Chembo ,\ title title Stability analysis of the spatiotemporal Lugiato - Lefever model for Kerr optical frequency combs in the anomalous and normal dispersion regimes , \ 10.1103/Phy...

  35. [43]

    Macnaughtan , author M

    author author M. Macnaughtan , author M. Erkintalo , author S. Coen , author S. Murdoch , \ and\ author Y. Xu ,\ title title Temporal characteristics of stationary switching waves in a normal dispersion pulsed-pump fiber cavity , \ 10.1364/OL.492998 journal journal Optics Lett...

  36. [44]

    author author T. J. \ Kippenberg , author A. L. \ Gaeta , author M. Lipson , \ and\ author M. L. \ Gorodetsky ,\ title title Dissipative Kerr solitons in optical microresonators , \ 10.1126/science.aan8083 journal journal Science \ volume 361 ,\ pages eaan8083 ( year 2018 ) NoStop

  37. [45]

    Englebert , author C

    author author N. Englebert , author C. M. \ Arabí , author S.-P. \ Gorza , \ and\ author F. Leo ,\ title title High peak-to-background-ratio solitons in a coherently driven active fiber cavity , \ 10.1063/5.0159693 journal journal APL Photonics \ volume 8 ,\ pages 120802 ( yea...

  38. [46]

    author author D. C. \ Cole , author A. Gatti , author S. B. \ Papp , author F. Prati , \ and\ author L. Lugiato ,\ title title Theory of kerr frequency combs in fabry-perot resonators , \ @noop journal journal Physical Review A \ volume 98 ,\ pages 013831 ( year 2018 ) NoStop

  39. [47]

    Ziani , author T

    author author Z. Ziani , author T. Bunel , author A. M. \ Perego , author A. Mussot , \ and\ author M. Conforti ,\ title title Theory of modulation instability in Kerr Fabry-Perot resonators beyond the mean-field limit , \ 10.1103/PhysRevA.109.013507 journal journal Physical R...

  40. [48]

    Cai , author R

    author author Y. Cai , author R. Sohanpal , author Y. Luo , author A. M. \ Heidt , \ and\ author Z. Liu ,\ title title On the design of low phase noise and flat spectrum optical parametric frequency comb , \ 10.1063/5.0165775 journal journal APL Photonics \ volume 8 ,\ pages 1...

  41. [49]

    Rubiola \ and\ author F

    author author E. Rubiola \ and\ author F. Vernotte ,\ title title The Companion of Enrico ’s Chart for Phase Noise and Two - Sample Variances , \ 10.1109/TMTT.2023.3238267 journal journal IEEE Transactions on Microwave Theory and Techniques \ volume 71 ,\ pages 2996--3025 ( ye...

  42. [50]

    Kuznetsov , author A

    author author N. Kuznetsov , author A. Nardi , author A. Davydova , author M. Churaev , author J. Riemensberger , author P. Seidler , \ and\ author T. J. \ Kippenberg ,\ http://arxiv.org/abs/2404.08609 title An ultra-broadband photonic-chip-based traveling-wave parametric ampl...

  43. [51]

    Riemensberger , author N

    author author J. Riemensberger , author N. Kuznetsov , author J. Liu , author J. He , author R. N. \ Wang , \ and\ author T. J. \ Kippenberg ,\ title title A photonic integrated continuous-travelling-wave parametric amplifier , \ 10.1038/s41586-022-05329-1 journal journal Natu...

  44. [52]

    Xu , author Y

    author author Y. Xu , author Y. Lin , author A. Nielsen , author I. Hendry , author S. Coen , author M. Erkintalo , author H. Ma , \ and\ author S. G. \ Murdoch ,\ title title Harmonic and rational harmonic driving of microresonator soliton frequency combs , \ 10.1364/OPTICA.3...

Pith tools

Reviewed August 8, 2026 · model on record in the stance chip above.