
Researchers at the École Polytechnique Fédérale de Lausanne (EPFL) Hybrid Photonics Laboratory and Center for Quantum Science and Engineering have demonstrated an integrated electro-optic transducer bridging the millimeter-wave (mm-wave) and telecom optical domains. Detailed in the paper “Coherent transduction and dynamical back-action between light and millimeter waves,” the architecture couples a thin-film lithium niobate (TFLN) photonic molecule to a sub-millimeter metallic resonator, achieving a vacuum electro-optic coupling rate of approximately 60 kHz and an internal conversion efficiency of 67%.
| EPFL Integrated Millimeter-Wave-to-Optical Transducer Specifications | ||
|---|---|---|
| Parameter | Measured Value | Architectural Significance |
| Operating Frequencies | 263 GHz (mm-wave) / 192 THz (1,561 nm telecom optical) | Interfaces high-frequency cryogenic modes and atomic Rydberg transitions directly with telecom C-band optical infrastructure. |
| Optical Resonators | Coupled Fabry–Pérot cavities in TFLN (lengths 110 μm and 119 μm) | Achieves free spectral ranges exceeding 650 GHz with optical quality factors up to 106 (κ± / 2π ≈ 186–230 MHz). |
| Electromagnetic Resonator | Quarter-wave gold resonator (length ≈ 165 μm) | Replaces macroscopic lines to equalize optical and mm-wave mode volumes, eliminating spatial overlap penalties. |
| Vacuum Coupling Rate (g0 / 2π) | 60 ± 8 kHz | Scales g0 linearly with frequency, exceeding microwave-domain electro-optic coupling rates by a factor of 60. |
| Electro-Optic Cooperativity (C) | Up to 0.27 ± 0.03 | Yields 67% internal photon conversion efficiency and drives observable dynamical back-action linewidth modulation. |
| Effective Thermal Detection | 0.21 ± 0.08 photons | Resolves thermal background occupancies below the single-quantum limit directly via optical sideband detection. |
Coherent frequency conversion between high-frequency electric fields and optical carriers serves as a critical interface for distributed quantum architectures, linking cryogenic processors and neutral-atom registers over optical fiber without introducing thermal load. While vacuum electro-optic coupling scales with operating frequency according to g0 ∝ (ωmmw / Vmmw)1/2, conventional implementations suffered from mode-volume mismatch: sub-millimeter electromagnetic fields were paired with millimeter-scale optical racetrack resonators, degrading field overlap and reducing net cooperativity.
The EPFL design resolves this spatial discrepancy by defining two compact Fabry–Pérot microcavities via photonic crystal mirrors etched into a suspended 400 nm TFLN membrane. Integrated DC tuning electrodes adjust the residual detuning between the resulting symmetric and anti-symmetric modes to align the doublet splitting with the adjacent quarter-wavelength resonator. Complete polarization alignment along the crystalline Z-axis maximizes interaction with lithium niobate’s primary Pockels tensor component (r33).
Because the optical linewidth is roughly two orders of magnitude narrower than the dissipative mm-wave resonance (γmmw / 2π ≈ 15 GHz), the transducer operates in the reversed dissipation regime (κ± ≪ γmmw). The optical filter isolates the narrow spectral slice of room-temperature thermal mm-wave photons falling within its bandwidth, enabling the thermal sideband to function as an uncalibrated internal standard for measuring device cooperativity.
Under coherent drive, electro-optic dynamical back-action modulates the optical response: the beam-splitter up-conversion interaction introduces an additional dissipation path that broadens the optical linewidth, while parametric down-conversion anti-damps and narrows the mode. Although total off-chip wireless efficiency remains constrained by free-space beam coupling into the integrated antenna (1.6 × 10−4), transitioning from a normal-metal gold resonator to high-gap superconductors such as niobium titanium nitride (NbTiN) is projected to suppress internal ohmic damping and increase total transduction efficiency at liquid-helium temperatures.
The research is detailed in the technical preprint here.
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