PPLN Λ = 18.99 µm · 1550 → 775 nm · 2 px/µm

6.1 Electro-optic modulators

L1 Phenomenon

A modulator is an interferometer whose arms are built in a Pockels crystal. A voltage across one or both arms changes the refractive index, shifts the phase of the light in that arm, and moves the output between bright and dark. Thin-film LN confines light to a sub-micron ridge, so the gold electrodes can sit a few microns apart (median gap 5.0 µm over 144 TFLN device rows derived); the same index change then needs a few volts, and the electrodes can carry a microwave signal along the chip at nearly the speed of the light.

MZM bench: transfer T(V) and optical eyefirst-order drive low-pass at f3dB; PRBS9
−4−202400.250.50.751drive voltage V (V)transmission TVπ
Vπ  2.00 Vbias  −90.0° Vpp/Vπ 0.50ER   7.7 dB Δφ  −90.0° ±  45.0°eye height 0.66baud/f3dB  1.00
103 rows
 2.00 V
100 GHz
 −90°
 1.00 V
100 GBd
Format
Vπ and f3dB are display templates; pick an atlas row to load measured values.
Drag the bias; set drive swing and symbol rate; switch NRZ / PAM4.

Die: Li 2026 (device d) geometry from eo-modulator-atlas (9 mm G-S-G line, x-cut) reported; output arm brightness follows T at the bias point; light at 1550 nm in false color. Drag to orbit.

−4−202400.250.50.751drive voltage V (V)transmission TVπ
100 GBd
 1.00 V
 −90°
100 GHz
 2.00 V
Format
Arm phase difference Δφ (bias ± swing)
 −90.0° ±  45.0°
Eye height (of T = 0..1)
0.66
Static extinction
  7.7 dB
Vpp / Vπ
0.50
Symbol rate / f3dB
 1.00
Vπ and f3dB are display templates; pick an atlas row to load measured values.model: PRBS9 drive, first-order low-pass, T = cos2(πV/2Vπ + φb/2) derived

L2 Transfer function, VπL, families

Transfer function and half-wave voltage

Mach-Zehnder intensity transfer (lossless, balanced splitters):

T(V)=12[1+cos(πVVπ+φb)]
  • Vπ is the voltage that moves T from maximum to minimum; φb is the static bias phase.
  • Push-pull drive puts opposite fields in the two arms; one signal electrode between two grounds (G-S-G) does this on x-cut film. For the same electrode, the push-pull MZM Vπ is half the single-arm phase-shifter Vπ.
  • IQ modulator: two MZMs nested in an outer interferometer with a 90-degree phase between them; each child MZM is biased at null.

Half-wave voltage-length product for an x-cut film, TE mode, field along the crystal z axis:

VπL=λg2ne3r33Γ(push-pull MZM)
  • g: electrode gap; Γ: overlap between the normalized optical intensity and the applied field Ez (Γ = (g/V) integral of Ez |Eopt|2 dA / integral of |Eopt|2 dA). The full tensor overlap is evaluated by the eo-modulator-atlas FEM engine (chapter 2.2, L3).
  • Worked value: λ = 1.55 µm, g = 5 µm template, Γ = 0.5 template, ne = 2.1376 at 1550 nm, 21 C derived, r33S = 30.8 pm/V at 633 nm P-comp (Turner 1966 via Weis and Gaylord Table 4): VπL = 2.58 V cm derived.
  • r33 choice moves the result: the Kaminow 1980 value 28.8 pm/V P-comp gives 2.75 V cm derived (+7%). No primary r33 measurement at 1550 nm is available; the 633 nm clamped value is used.
  • Atlas cross-check: median telecom push-pull VπL for TFLN MZM/IQ device rows is 2.44 V cm (n = 66 rows) derived: eo-modulator-atlas device rows at commit eb97f96, telecom band, push-pull convention, MZM and IQ.
VπL = λg / (2 ne3 r33 Γ), push-pull, x-cut TE71 atlas rows
g = 5.0 µm5 µmvertical ×8SiO2LN, x-cut
02.557.51012.5150.1110electrode gap g (µm)implied overlap Γlateral-gap model not applicable (Γ > 1)
VπL  2.58 V cmne 2.1376 Γ 0.50vs 1.55 µm × 1.00
 5.0 µm
0.50
1.550 µm
r33 source
P-comp
Scatter y axis
r33: 633 nm clamped values (no primary 1550 nm value in the sources held). ne(λ): Zelmon 1997, 21 C P-db. Scatter: Γimplied = λg / (2 ne3 r33 VπL) per atlas row derived; hollow: slow light, material-enhancement claim, hybrid Si/SiN, unetched LN; rows within 12% of λ in full tone; crosshair = slider state.atlas eb97f96 · 2026-10-20 · fetched 2026-10-25
g = 5.0 µm5 µmvertical ×8SiO₂LN, x-cut
VπL, push-pull 2.58 V cm
ne at λ (Zelmon 1997)
2.1376
r33 (633 nm, clamped)
30.8 pm/V
Reduction vs 1.55 µm
× 1.00
1.550 µm
 5.0 µm
0.50
r33 source
024681012140.1110electrode gap g (µm)implied overlap Γlateral-gap model not applicable (Γ > 1)
Gap and overlap are templates template; r33 P-comp; mode drawn at 1550 nm in false color, vertical scale exaggerated. Scatter: Γimplied = λg / (2 ne3 r33 VπL) for 71 x-cut push-pull TFLN rows derived, ne from Zelmon 1997 at 21 C P-db; the shaded region Γ > 1 is outside the lateral-gap model. Hollow: slow light, material-enhancement claim, hybrid Si/SiN, unetched LN; rows within 12% of the chosen wavelength in full tone; crosshair = slider state.atlas eb97f96 · 2026-10-20 · fetched 2026-10-25

Implied overlap from the atlas (derived): over 71 x-cut TFLN push-pull MZM/IQ device rows with gap, wavelength, and VπL, Γimplied spans 0.15 to 6.12, with 45 of 71 rows between 0.45 and 0.67 derived. Values above 1 are not physical overlaps; 8 rows exceed 1 and mark devices outside the lateral-gap model or its inputs: four operating points of the Shen 2024 slow-light MZM (6.12, 3.21, 1.84, 1.31), two Yu 2024 devices that claim a material enhancement (1.33, 1.47), and two Xue 2026 devices (1.03, capacitively loaded, thick silica buffer). The formula assumes the 633 nm clamped r33 at all wavelengths and Zelmon ne at the row wavelength.

Modulator families

FamilyHow it worksAtlas TFLN device rows (by electrode type or device class)Representative device, values
Lumped electrodeElectrode shorter than the RF wavelength; RC-limitedlumped 26Wang 2018 (Opt. Express) rings; see the ring table below
Traveling-wave CPW / GSGElectrode is a transmission line co-propagating with the lightGSG 72, CPW 20, GSSG 8CMOS-compatible drive, up to 210 Gb/s, on-chip loss < 0.5 dB reported
Capacitively loaded (T-rail) traveling waveSmall T-shaped segments reach toward the waveguide; current flows in rails away from the gapcapacitively loaded 32RF Vπ 1.3 V with 1.8 dB roll-off at 50 GHz reported
Slow-wave electrodePeriodic loading raises the RF index to match a high optical group indexslow wave 150.21 V cm, 1 mm, slow-light SiN-loaded TFLN, bandwidth > 110 GHz reported
Ridge-top transparent electrodesConductive oxide on the ridge, field across the filmnot counted (no atlas class)0.33 V cm, 300 µm; 2.4 dB roll-off at 110 GHz; 3 dB bandwidth 145 GHz extrapolated; on-chip IL 2.7 dB reported
IQ modulatorNested MZMsIQ 10dual-polarization IQ, sub-1-V drive, 110 GHz, 1.96 Tb/s net single wavelength reported
Ring / photonic-crystal resonatorResonance shifted by Pockels effect; photon lifetime limits speedring 15, other resonator 16see below
Heterogeneous Si or SiN + bonded LNLight in Si/SiN, mode partly in LN; LN unetchedbonded heterogeneous 26 (all TFLN rows)110 GHz, 110 mW optical power, hybrid Si-LN reported; Si/LN MZM for 100 Gbit/s reported

Counts: 209 TFLN device rows at atlas commit eb97f96 derived; 31 rows have no electrode type.

Ring and photonic-crystal modulators

Resonance shift per volt: Δ λ = λ Δ neff / ng. A resonator stores light for the photon lifetime τ = QL / ω0, so its modulation response rolls off on the scale of the linewidth Δ ν = ν0 / QL; the exact factor depends on detuning.

DeviceQL3 dB bandwidthNoteSource
TFLN ring, Q 5,7005,70040 GHzreported
TFLN ring, Q 8,0008,00030 GHzQ approximate in sourcereported
TFLN ring, Q 18,00018,00011 GHzreported
PhC cavity14,000 (approx.)17.5 GHz (approx.)photonic-crystal modulatorreported
Topological PhC, 64 µm electrode2,200> 110 GHz220 GBd NRZ eyereported

The Lorentzian linewidth ν0/QL at 1550 nm is 34 GHz for QL = 5,700 and 10.7 GHz for QL = 18,000 derived; measured bandwidths can exceed it when the device is operated detuned (atlas note on Zhang 2023 (b): headline 104 GHz at the -8 dB detuning point, authors' photon-lifetime limit 35 GHz).

Ring modulator, all-pass, critical coupling, 1550 nm13 atlas rows
−300−200−100010020030000.250.50.751wavelength offset (pm)transmission Tlaser
100010000100000106110100loaded Q3 dB EO bandwidth (GHz)ν0/QL at 1550 nm: linewidth, not a bound
QL   10000linewidth  19.34 GHz τph   8.23 psshift    0.0 pmT at laser 0.500
  10000
 7.0 pm/V
 0.00 V
−0.50 Δν
Linewidth ν0/QL, photon lifetime QL/(2πν0) derived. Tuning default 7 pm/V; the Wang 2018 Q 50,000 ring reports 0.007 nm/V reported. Ring radius 100 µm and ng 2.3 set the FSR only template. Detuning in linewidths of the unbiased resonance. Right plot: filled = EO S21, hollow = photon-lifetime estimate, arrow = lower bound; dashed line = linewidth.atlas eb97f96 · 2026-10-20 · fetched 2026-10-25
in, 1550 nmout: T = 0.500Au
  10000
 0.00 V
−0.50 Δν
Linewidth (speed scale)
 19.34 GHz
Photon lifetime
  8.23 ps
Resonance shift
   0.0 pm
T at the laser
0.500
−300−200−100010020030000.250.50.751wavelength offset (pm)transmission Tlaser
100010000100000106110100loaded Q3 dB EO bandwidth (GHz)ν0/QL at 1550 nm: linewidth, not a bound
Tuning 7 pm/V template; the Wang 2018 Q 50,000 ring reports 0.007 nm/V reported. Ring radius 100 µm and ng 2.3 set the FSR only template. Linewidth ν0/QL and photon lifetime QL/(2πν0) derived. The ring glow is the computed circulating power at the laser, in false color. Right: 13 atlas resonant modulators; filled = EO S21, hollow = photon-lifetime estimate, arrow = lower bound; dashed line = linewidth.atlas eb97f96 · 2026-10-20 · fetched 2026-10-25

L3 How Vπ and bandwidth are measured

How Vπ and bandwidth are measured, and why papers disagree

  • Convention. Vπ can be quoted per phase-shifter arm, for a push-pull MZM, or as a differential (V+ minus V-) value; these differ by factors of 2. Values are kept in the convention each paper states; none are converted. Example: the authors of Aimone 2026 (a) quote 1.1 V cm (differential reference); 3.26 V × 7.5 mm gives 2.45 V cm derived.
  • Frequency. Vπ measured below 1 GHz (DC, kHz or MHz triangle) and at RF differ: below about 20 kHz, charge relaxation in TFLN enhances the low-frequency response (relaxation-enhanced band 1-20 kHz, response measured 1 mHz to 1 MHz) reported. Vπ values are split at 1 GHz into DC and RF values.
  • Bandwidth reference. "3 dB EO bandwidth" is 20 log10 of the detected modulation amplitude relative to a stated reference (DC, 1 GHz, or an unstated low-frequency plateau). Methods differ: VNA/LCA EO S21, optical sideband ratio, link EOE response.
  • Instrument limits. 67 of 145 TFLN/TFLT bandwidth values in the atlas are lower bounds ("over 67 GHz", "over 110 GHz"); the most frequent bound values are 110 GHz (15 rows), 67 GHz (13), 50 GHz (12) derived. Medians over bounded data understate true bandwidth.
  • Extrapolation. Several headline bandwidths are extrapolated beyond the measured range (e.g. 220 / 218 GHz for C / O band at 7 mm, extrapolated reported). Extrapolated bandwidths are a separate class from measured ones.
  • Disclosure. Of 209 TFLN device rows, VπL is stated or derivable in 64%, 3 dB bandwidth in 60%, on-chip insertion loss in 25%, RF loss in 11%, Z0 in 10%, nRF in 10% derived.

Sources

14 cited in 6.1
RefTitleLink
Chen et al. 2025Ultra‐Compact and Ultra‐High Speed Topological Photonic Crystal Modulator Based on Thin Film Lithium Niobatedoi:10.1002/lpor.202500380
He et al. 2019High-performance hybrid silicon and lithium niobate Mach–Zehnder modulators for 100 Gbit s−1 and beyonddoi:10.1038/s41566-019-0378-6
Holzgrafe et al. 2024Relaxation of the electro-optic response in thin-film lithium niobate modulatorsdoi:10.1364/OE.507536
Kharel et al. 2021Breaking voltage–bandwidth limits in integrated lithium niobate modulators using micro-structured electrodesdoi:10.1364/OPTICA.416155
Li et al. 2020Lithium niobate photonic-crystal electro-optic modulatordoi:10.1038/s41467-020-17950-7
Liu et al. 2025Ultrahigh‐Efficiency Dual‐Band Thin‐Film Lithium Niobate Modulator Incorporating Low‐k Underfill for 390 Gbit s −1 PAM8 Transmissiondoi:10.1002/lpor.202402053
Shen et al. 2024Highly Efficient Slow‐Light Mach–Zehnder Modulator Achieving 0.21 V cm Efficiency with Bandwidth Surpassing 110 GHzdoi:10.1002/lpor.202401092
Valdez et al. 2022110 GHz, 110 mW hybrid silicon-lithium niobate Mach-Zehnder modulatordoi:10.1038/s41598-022-23403-6
Wang et al. 2018Integrated lithium niobate electro-optic modulators operating at CMOS-compatible voltagesdoi:10.1038/s41586-018-0551-y
Wang et al. 2018Nanophotonic lithium niobate electro-optic modulatorsdoi:10.1364/oe.26.001547
Weis and Gaylord 1985Lithium niobate: Summary of physical properties and crystal structuredoi:10.1007/BF00614817
Xu et al. 2022Dual-polarization thin-film lithium niobate in-phase quadrature modulators for terabit-per-second transmissiondoi:10.1364/OPTICA.449691
Yu et al. 20250.33 V · cm thin-film lithium niobate Mach-Zehnder modulator with ridge-top transparent electrodedoi:10.1364/oe.572384
Zelmon et al. 1997Infrared corrected Sellmeier coefficients for congruently grown lithium niobate and 5 mol% magnesium oxide –doped lithium niobatedoi:10.1364/JOSAB.14.003319