Reconfigurable Electro-Optic Comb Generator

• Reconfigurable electro‐optic comb generators are frequency comb sources that use programmable electrical control to tailor spectral properties such as repetition rate, bandwidth, and flatness.
• They achieve tunability by adjusting RF drive conditions, enabling dynamic control over comb line count, spectral envelope, and temporal pulse patterns.
• Demonstrations in silicon, lithium niobate, and other platforms highlight advances in power efficiency, hybrid EO–Kerr regimes, and reconfigurable microwave–optical co-design.

A reconfigurable electro-optic comb generator is an electro-optic frequency-comb source whose comb structure is controlled by electrical drive conditions rather than fixed solely by cavity geometry or mode-locking dynamics. Across current implementations, reconfigurability encompasses the ability to change comb repetition rate, optical bandwidth, number of lines, spectral flatness, overall envelope, temporal pulse pattern, and operating wavelength by varying radio-frequency or microwave waveforms, detuning, bias, or nonlinear-conversion conditions (Weckenmann et al., 2023, Song et al., 29 Jul 2025, Zhang et al., 2022, Didier et al., 15 Jun 2026). In integrated platforms, this function has been realized in silicon ring resonator modulators, thin-film lithium niobate and lithium tantalate microresonators, non-resonant multi-pass lithium-niobate modulators, Ge-rich SiGe Schottky modulators at $8\,\mu\text{m}$, and mid-infrared nonlinear-conversion architectures that map a telecom-band electro-optic comb into the mid-infrared (Weckenmann et al., 2023, Zhang et al., 2018, Hu et al., 2021, Chen et al., 2024, Zhang et al., 2024, Turpaud et al., 2024, Didier et al., 15 Jun 2026).

1. Definition and distinguishing characteristics

The defining feature of a reconfigurable electro-optic comb generator is that the comb is set by programmable electrical control. In a silicon ring resonator modulator, reconfigurability means the ability to change the number of comb lines $N_l$, spectral flatness, and overall spectral envelope by tuning harmonic amplitudes, phases, $V_{\mathrm{dc}}$, and laser–resonance detuning $\Delta\lambda$ (Weckenmann et al., 2023). In programmable cavity electro-optic combs on thin-film lithium niobate, the structure is controlled entirely by microwave waveforms, with reconfiguration of repetition rate, bandwidth, line-power distribution, and temporal pulse patterns (Song et al., 29 Jul 2025). In non-resonant lithium-niobate systems, reconfigurability is associated with excellent tunability in repetition rate and operation wavelength, and with waveform-dependent comb shaping (Zhang et al., 2022). In mid-infrared integrated systems based on nonlinear conversion, reconfigurability includes independent electronic control of both center wavelength and comb spacing (Didier et al., 15 Jun 2026).

Electro-optic combs differ from Kerr combs and mode-locked lasers in the way the line spacing is established. In resonant electro-optic combs, the optical pump undergoes multiple electro-optic modulation processes in a high-Q optical resonator, resulting in cascaded spectral sidebands, while the repetition rate is set by the microwave drive and the optical free spectral range (Chen et al., 2024, Zhang et al., 2024). In non-resonant systems, the repetition rate is simply the RF drive frequency, which can be widely tuned (Zhang et al., 2022). This suggests that the term “reconfigurable” is especially appropriate for electro-optic combs because the principal control parameters are electrical and can be changed without replacing the optical hardware (Eliason et al., 2024, Song et al., 29 Jul 2025).

A persistent misconception is that cavity electro-optic combs are adequately described only by nearest-neighbor mode coupling. The 2025 thin-film lithium niobate work explicitly states that, in the strong-coupling regime, the coupling is not limited to nearest neighbors and instead forms complete long-range connectivity in frequency space (Song et al., 29 Jul 2025). Another misconception is that high-quality comb flattening necessarily requires multi-stage external pulse-shaping hardware. A single silicon ring resonator modulator driven by harmonically optimized RF waveforms synthesized 7-line and 9-line combs with measured power imbalance of $2.9\,\text{dB}$ and $5.4\,\text{dB}$, respectively, compared to $9.4\,\text{dB}$ for an optimized 5-line comb generated from a single sinusoidal driving signal (Weckenmann et al., 2023).

2. Physical principles of electro-optic comb formation

Electro-optic comb generation begins with a continuous-wave optical field subjected to periodic modulation. For a single phase modulator driven sinusoidally at frequency $f_m$, the optical field can be written as

$$E(t) = E_0\,e^{i(2\pi \nu_0 t + \beta \sin 2\pi f_m t)},$$

which expands into discrete tones at $\nu_0 + n f_m$ with amplitudes proportional to $N_l$0 (Ruiz-Llata et al., 2023). The same phase-modulation description appears in integrated lithium-niobate and silicon implementations, where the modulation index or resonant enhancement determines the number of significant sidebands (Zhang et al., 2018, Zhang et al., 2022).

In resonant ring or racetrack devices, the phase modulation is filtered by the cavity. In a silicon all-pass ring resonator modulator, the resonance condition is

$N_l$1

with free spectral range approximately

$N_l$2

and the output field is

$N_l$3

where the periodically varying round-trip phase $N_l$4 is controlled by carrier depletion in a lateral PN junction (Weckenmann et al., 2023). In thin-film lithium niobate resonators, driving at a microwave frequency equal to the free spectral range causes coherent energy transfer between adjacent cavity modes and produces a resonantly enhanced electro-optic comb (Zhang et al., 2018, Chen et al., 2024, Zhang et al., 2024).

In strong cavity electro-optic coupling, the most useful description is a synthetic frequency lattice. The thin-film lithium niobate cavity work models the intracavity amplitudes $N_l$5 through

$N_l$6

where the effective couplings $N_l$7 are determined by modulation depths and microwave phases (Song et al., 29 Jul 2025). For single-tone operation, higher-order couplings become important when $N_l$8, and the comb transitions between distinct pulse-number states as modulation depth is increased (Song et al., 29 Jul 2025).

The same synthetic-lattice picture also underpins triply resonant lithium tantalate devices. There, the EO interaction is described by

$N_l$9

with effective coupling $V_{\mathrm{dc}}$0 under strong microwave drive (Zhang et al., 2024). A plausible implication is that “reconfigurable” in cavity electro-optic systems increasingly refers not only to line spacing control but also to programmable engineering of the coupling graph itself (Song et al., 29 Jul 2025, Zhang et al., 2024).

3. Device classes and material platforms

A first major class is the silicon ring resonator modulator. The device reported in 2023 is an all-pass ring resonator with a carrier-depletion phase-shifter implemented as a lateral PN junction in the ring waveguide, with $V_{\mathrm{dc}}$1, loaded $V_{\mathrm{dc}}$2, and optical linewidth of about $V_{\mathrm{dc}}$3 (Weckenmann et al., 2023). Its distinctive feature is reconfigurable comb flattening through harmonic superposition of the RF drive.

A second class is the integrated resonant thin-film lithium niobate comb. A single TFLN microring with integrated electrodes produced more than the entire telecommunications L-band, over 900 comb lines spaced at $V_{\mathrm{dc}}$4, and exhibited frequency spacing finely controllable over seven orders of magnitude, from $V_{\mathrm{dc}}$5 to $V_{\mathrm{dc}}$6, in dual-comb operation (Zhang et al., 2018). Microwave-resonator-enabled TFLN devices later replaced the lumped-capacitor electrode with a quarter-wave coplanar microwave resonator, achieving more than three times electrical power reduction with minimal reflection and a comb span of $V_{\mathrm{dc}}$7 at $V_{\mathrm{dc}}$8 (Chen et al., 2024).

A third class is the coupled-resonator TFLN comb. The 2021 coupled micro-resonator architecture uses a pump coupling cavity and a comb cavity to satisfy generalized critical coupling,

$V_{\mathrm{dc}}$9

thereby decoupling bandwidth from efficiency (Hu et al., 2021). That device achieved $\Delta\lambda$0 pump-to-comb conversion efficiency and $\Delta\lambda$1 bandwidth at $\Delta\lambda$2 pump power, and $\Delta\lambda$3 bandwidth in a combined EO–$\Delta\lambda$4 regime at higher pump power (Hu et al., 2021).

A fourth class is the triply resonant lithium tantalate architecture. By combining a LiTaO$\Delta\lambda$5 optical racetrack resonator, a monolithic microwave resonator, and a hybrid-integrated laser diode, the 2024 work reported a four-fold comb span extension and a 16-fold power reduction compared to the conventional non-resonant microwave design, reaching over $\Delta\lambda$6 and $\Delta\lambda$7 with $\Delta\lambda$8 lines in a $\Delta\lambda$9 footprint (Zhang et al., 2024).

A fifth class is the non-resonant multi-pass lithium-niobate modulator. Passing optical signals through the modulation electrodes for a total of 4 round trips reduced electrical power consumption by more than one order of magnitude and produced 47 comb lines at a 25-GHz repetition rate using $2.9\,\text{dB}$0 RF power (Zhang et al., 2022). This non-resonant architecture emphasizes tunability of repetition rate and operation wavelength rather than cavity enhancement (Zhang et al., 2022).

A sixth class is the hybrid microcomb plus electro-optic modulation architecture. Interleaving electro-optic sidebands with a parametric microcomb enabled direct control and stabilization of a microcomb spectrum with large mode spacing $2.9\,\text{dB}$1, achieving a residual 1-second-instability of $2.9\,\text{dB}$2 and a microwave-reference-limited absolute instability of $2.9\,\text{dB}$3 at $2.9\,\text{dB}$4 mode spacing (Del'Haye et al., 2012). This architecture is reconfigurable in the sense that EO spacing and subharmonic locking define a new effective comb spacing (Del'Haye et al., 2012).

A seventh class extends electro-optic comb generation into the mid-infrared. A Ge-rich graded SiGe Schottky modulator generated electro-optical combs spanning over $2.9\,\text{dB}$5 around $2.9\,\text{dB}$6 by using harmonically rich RF signals to compensate limited modulator efficiency (Turpaud et al., 2024). A later thin-film lithium-niobate architecture generated a mid-infrared EO comb through difference-frequency generation in PPLN, with approximately $2.9\,\text{dB}$7 bandwidth and center wavelength tunability of over $2.9\,\text{dB}$8, and demonstrated dual-tone EO comb generation in the mid-infrared (Didier et al., 15 Jun 2026). A 2026 free-space ultrafast modulator at $2.9\,\text{dB}$9 further realized single- and dual-comb operation from a continuous-wave quantum cascade laser with tunable repetition rates down to the megahertz range (Ngo et al., 3 Jul 2026).

4. Reconfiguration mechanisms and control strategies

The most direct reconfiguration mechanism is microwave waveform design. In the silicon ring resonator modulator, the drive voltage is

$5.4\,\text{dB}$0

A differential evolution algorithm optimizes $5.4\,\text{dB}$1 to minimize the unbiased sample variance of comb line powers (Weckenmann et al., 2023). The power imbalance metric is

$5.4\,\text{dB}$2

and the fitness function is

$5.4\,\text{dB}$3

with $5.4\,\text{dB}$4 the mean line power (Weckenmann et al., 2023). This approach makes explicit that “reconfigurable” can mean software-defined flattening objectives rather than only hardware retuning (Weckenmann et al., 2023).

A broader microwave-programmability paradigm appears in cavity electro-optic combs. The 2025 TFLN work uses

$5.4\,\text{dB}$5

and, for multi-tone modulation,

$5.4\,\text{dB}$6

to engineer complete long-range connectivity in the frequency lattice (Song et al., 29 Jul 2025). By choosing $5.4\,\text{dB}$7, the device can boost bandwidth, flatten spectra, impose desired spectral envelopes, and control temporal pulse patterns (Song et al., 29 Jul 2025). The same work achieved a waveform approximating a square wave up to the 7th harmonic, which yielded approximately 457 comb modes and $5.4\,\text{dB}$8 pulses versus 216 modes and $5.4\,\text{dB}$9 for single-tone drive at fixed total RF power (Song et al., 29 Jul 2025).

Non-resonant systems expose similar but often more transparent control knobs. In the 2022 multi-pass lithium-niobate modulator, repetition rate is tuned by RF frequency, center wavelength by the seed laser, and bandwidth by RF power, while maximal efficiency recurs every $9.4\,\text{dB}$0 because of RF–optical phase matching (Zhang et al., 2022). In the 2024 cascaded harmonic architecture, three phase modulators are driven at sequentially lower harmonics, and the lowest modulation frequency sets the repetition rate while higher harmonics determine spectral filling (Eliason et al., 2024). In the computational spectroscopy work, the phase modulator is driven with a sequence of waveforms

$9.4\,\text{dB}$1

with

$9.4\,\text{dB}$2

so that each RF configuration generates a known probe comb for solving an inverse problem (Navarro-Alventosa et al., 18 Sep 2025). This suggests a general distinction between waveform-programmable EO comb generators, which optimize a succession of spectra, and state-programmable cavity EO comb generators, which navigate a nonlinear state space controlled by modulation depth and detuning (Navarro-Alventosa et al., 18 Sep 2025, Song et al., 29 Jul 2025).

5. Representative demonstrations and performance regimes

Flatness optimization in a single silicon ring resonator modulator is a compact demonstration of reconfigurable spectral synthesis. With a single sinusoidal drive at $9.4\,\text{dB}$3, $9.4\,\text{dB}$4 peak-to-peak, and $9.4\,\text{dB}$5, the minimum power imbalance for 5 lines was $9.4\,\text{dB}$6 (Weckenmann et al., 2023). With harmonic superposition and experimentally constrained conditions, the same device produced a 7-line comb with $9.4\,\text{dB}$7 and a 9-line comb with $9.4\,\text{dB}$8, both centered at the CW frequency with $9.4\,\text{dB}$9 spacing (Weckenmann et al., 2023).

Programmable cavity EO combs on thin-film lithium niobate demonstrate a qualitatively different regime. In a device with $f_m$0, EO bandwidth $f_m$1, and modulation at harmonics of the FSR, the number of comb modes was approximately conserved at $f_m$2 for 4, 5, and 7 FSR repetition-rate operation, while total span scaled from $f_m$3 to $f_m$4 (Song et al., 29 Jul 2025). The same work also realized flat-top combs with slope $f_m$5 over $f_m$6 modes and less than $f_m$7 variation across more than 100 lines at moderate RF power by introducing synthetic frequency boundaries through microwave detuning (Song et al., 29 Jul 2025).

Power-efficient resonant architectures have substantially shifted the bandwidth–power frontier. The microwave resonator-enabled TFLN comb reached $f_m$8 span and approximately 430 lines at $f_m$9 or $$E(t) = E_0\,e^{i(2\pi \nu_0 t + \beta \sin 2\pi f_m t)},$$0, with $$E(t) = E_0\,e^{i(2\pi \nu_0 t + \beta \sin 2\pi f_m t)},$$1 at resonance and more than three times electrical power reduction relative to lumped-capacitor electrodes (Chen et al., 2024). The lithium tantalate triply resonant device further pushed span to over $$E(t) = E_0\,e^{i(2\pi \nu_0 t + \beta \sin 2\pi f_m t)},$$2 and $$E(t) = E_0\,e^{i(2\pi \nu_0 t + \beta \sin 2\pi f_m t)},$$3 with $$E(t) = E_0\,e^{i(2\pi \nu_0 t + \beta \sin 2\pi f_m t)},$$4 lines, while also exhibiting a comb existence range approaching the full free spectral range of the optical microresonator (Zhang et al., 2024).

Hybrid nonlinear regimes extend EO combs beyond purely electro-optic scaling. The coupled-resonator TFLN comb achieved $$E(t) = E_0\,e^{i(2\pi \nu_0 t + \beta \sin 2\pi f_m t)},$$5 conversion efficiency and $$E(t) = E_0\,e^{i(2\pi \nu_0 t + \beta \sin 2\pi f_m t)},$$6 bandwidth, and at higher optical power entered a combined EO–$$E(t) = E_0\,e^{i(2\pi \nu_0 t + \beta \sin 2\pi f_m t)},$$7 regime with $$E(t) = E_0\,e^{i(2\pi \nu_0 t + \beta \sin 2\pi f_m t)},$$8 bandwidth and $$E(t) = E_0\,e^{i(2\pi \nu_0 t + \beta \sin 2\pi f_m t)},$$9 pulse peak power (Hu et al., 2021). The self-locked Raman-electro-optic microcomb combined EO, Kerr, and Raman processes to generate nearly 1400 comb lines spanning over $\nu_0 + n f_m$0 with repetition rate $\nu_0 + n f_m$1, while maintaining a self-locked low-noise state without external active feedback (Wan et al., 2024). These results indicate that reconfigurability increasingly includes controlled access to hybrid EO–Kerr–Raman operating regimes rather than only tuning within a single linear EO model (Hu et al., 2021, Wan et al., 2024).

At the opposite end of the design space, non-resonant and application-driven architectures emphasize agile spacing and system matching. A dual electro-optic comb photonic thermometry system generated approximately 40 comb teeth within a 5 dB power-leveled range and $\nu_0 + n f_m$2 with $\nu_0 + n f_m$3, enabling a read-out stability of $\nu_0 + n f_m$4 at $\nu_0 + n f_m$5 (Fleisher et al., 2022). Dual-comb photoacoustic spectroscopy employed EO combs with $\nu_0 + n f_m$6 and $\nu_0 + n f_m$7, mapping a $\nu_0 + n f_m$8 optical span onto a $\nu_0 + n f_m$9 acoustic span and reconstructing ammonia absorption with $N_l$00 bandwidth and $N_l$01 resolution (Ruiz-Llata et al., 2023). In both cases, reconfigurability refers less to extreme bandwidth and more to electronic adaptation of comb spacing and offset to the response of the sensing instrument (Fleisher et al., 2022, Ruiz-Llata et al., 2023).

6. Applications, limitations, and future directions

Electro-optic comb reconfigurability has made these sources central to spectroscopy, microwave photonics, communications, and photonic computing. In spectroscopy, dual electro-optic combs simplify optimization of the multiheterodyne signal according to the characteristic of the detection module, as demonstrated in ammonia photoacoustic sensing (Ruiz-Llata et al., 2023). In thermometry, dual EO combs interrogated a $N_l$02-phase-shifted fiber Bragg grating with $N_l$03 stability at $N_l$04, and the authors explicitly described the EO generation scheme as scalable and reconfigurable (Fleisher et al., 2022). In computational spectroscopy, a reconfigurable EO comb generator produced a sequence of known probe spectra, enabling reconstruction from integrated power measurements acquired within $N_l$05 (Navarro-Alventosa et al., 18 Sep 2025).

In microwave photonics and optical computing, the most direct use of reconfigurability is as a programmable spectral weighting engine. A programmable EO comb on TFLN implemented image edge detection and object classification, provided near-unity optical power conversion efficiency, weight reconstruction speed exceeding $N_l$06, and a parallel convolution computing speed of $N_l$07 (He et al., 23 Jun 2025). The central point is that the same comb simultaneously serves as multi-wavelength source and weight bank (He et al., 23 Jun 2025). A plausible implication is that EO comb generators are evolving from optical sources into RF-defined photonic processors (He et al., 23 Jun 2025, Navarro-Alventosa et al., 18 Sep 2025).

The main technical limitations are also consistent across platforms. Resonant EO combs are constrained by the trade-off between optical $N_l$08, electrical bandwidth, dispersion, and RF power (Zhang et al., 2018, Chen et al., 2024). Non-resonant EO combs offer broad tuning but can require high RF power unless multi-pass or multi-tone enhancement is used (Zhang et al., 2022, Eliason et al., 2024). Model mismatch, electrical roll-off, amplifier linearity, AWG resolution, and simplified device models limit how precisely an optimized RF waveform maps to the desired comb (Weckenmann et al., 2023, Navarro-Alventosa et al., 18 Sep 2025). In thin-film lithium niobate, strong birefringence can distort mode spacing; the lithium tantalate triply resonant work addressed this with reduced birefringence and smoother integrated dispersion (Zhang et al., 2024).

Several directions now define the field’s trajectory. One is stronger microwave–optical co-design, exemplified by microwave resonators and triply resonant lithium tantalate circuits (Chen et al., 2024, Zhang et al., 2024). Another is broader programmability through multi-tone synthetic drives, inverse design, and machine-learning optimization (Song et al., 29 Jul 2025, He et al., 23 Jun 2025, Navarro-Alventosa et al., 18 Sep 2025). A third is spectral expansion into the mid-infrared, where Ge-rich SiGe modulators at $N_l$09, integrated DFG-based EO combs up to $N_l$10, and $N_l$11 free-space ultrafast modulators show that EO reconfigurability is no longer restricted to the telecom band (Turpaud et al., 2024, Didier et al., 15 Jun 2026, Ngo et al., 3 Jul 2026). This suggests that the mature definition of a reconfigurable electro-optic comb generator is no longer merely “an EO comb with tunable line spacing,” but an electrically programmable frequency-lattice system whose spectral and temporal output can be shaped across platforms, wavelength bands, and application domains (Song et al., 29 Jul 2025, Didier et al., 15 Jun 2026).