Photodetector & Optical Receiver Front-End

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last updated 2026-08-31 · +5 sources in last 30d
Assessment draft · unreviewed
Viability
5/5
Drivers
4/5
Novelty
4/5
Diffusion
3/5
Impact
4/5

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Germanium Photodiodes Germanium Photodiod… InGaAs Photodiodes InGaAs Photodiodes Avalanche Photodiode (APD / SPAD) Avalanche Photodiod… Co-Packaged Optics Co-Packaged Optics Optical Interconnect Optical Interconnect Silicon Photonics Silicon Photonics External Laser Source (ELS) for Co-Packaged Optics External Laser Sour… Uni-Traveling-Carrier Photodiode (UTC-PD) Uni-Traveling-Carri… Photodete…

The photodetector and its receiver front-end convert light back into electrical bits, and recent fabricated demonstrations, including a single-chip 1.024 Tb/s CMOS receiver at 71 fJ/b and a 206 GHz photodiode, show the receiver is now where much of the remaining energy and bandwidth headroom in optical links sits.

Summary

An optical receiver front-end is the input half of any optical link. A photodetector, usually a reverse-biased photodiode, converts incoming photons into a photocurrent; a transimpedance amplifier (TIA) turns that small current into a voltage swing large enough for a decision circuit or ADC. Everything that matters about a link’s power budget converges here: the detector’s responsivity in amps per watt, its 3 dB bandwidth, the parasitic capacitance between detector and amplifier, and the amplifier’s input-referred noise, which sets the minimum received optical power (sensitivity) for a given bit error rate.

The design tension is structural. Photodiode quantum efficiency and bandwidth trade against each other, because a thicker absorption region catches more light but slows carrier transit; work on modified uni-travelling-carrier (MUTC) photodiodes attacks this directly, with an InP waveguide-integrated device reaching a 206 GHz 3 dB bandwidth at 0.81 A/W external responsivity and a bandwidth-efficiency product above 130 GHz. The second tension is integration: detector and amplifier fabricated in different processes accumulate parasitics at the interface, which is the explicit motivation for 3D heterogeneous integration by micro-transfer printing of a 0.06 mm2 BiCMOS chiplet onto a silicon photonic IC, giving 224 Gb/s PAM-4 at minus 5.2 dBm OMA sensitivity and 0.51 pJ/b.

The parameters that decide the field are therefore: energy per bit, bandwidth density, sensitivity, and whether the front-end can be built in a commercial foundry flow. Two 2026 results set the current markers. A monolithic analogue front-end in the GlobalFoundries Fotonix platform achieves 28.9 GHz bandwidth and 61.7 dBohm gain at 9.22 mW and 0.08 pJ/bit, with under 737 nA RMS input-referred noise current and PAM-4 eyes measured to 64 GBaud. A 32-channel WDM receiver monolithically integrated in 45nm CMOS runs 1.024 Tb/s aggregate at 71 fJ/b including photonic tuning and control power, with 4 Tb/s/mm2 bandwidth density and BER below 1e-12 with no equalisation, error correction or DSP.

Outside data-centre links, the same component class is under pressure from three other directions: sub-THz wireless, where the photodiode is the photonic mixer generating RF power; mid-infrared sensing and free-space optics, where fast room-temperature detectors are scarce; and quantum systems, where the receiver choice determines what information survives measurement at all.

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Assessment drafted 2026-08-31 from up to 17 KB sources using the technology-scorecard framework; scores are a draft read pending review.

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