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Performance Benchmarks

This page provides detailed performance metrics for the Q-Memory photonic platform, organised by capability area. Figures marked as “projected” are engineering estimates based on published literature for comparable photonic systems; figures marked as “Phase 0 target” are validated through the Phase 0 fabrication run.

Silicon nitride waveguides are the primary photon-carrying medium. The target loss is:

PhaseLoss targetSignificance
Phase 0< 2 dB/cmValidates process quality; acceptable for proof-of-concept
Phase 1+< 0.5 dB/mRequired for fault-tolerant quantum operation

At 0.5 dB/m, a 10 cm photon path loses only 0.01% of its light — well within fault-tolerance budgets. Conventional silicon waveguides at ~2 dB/cm would lose far more over the same path, making them incompatible with fault-tolerant photonic quantum computing.

ParameterPhase 0 targetPhase 1 target
Power for π phase shift< 25 mW< 15 mW
Switching response time (thermal)< 10 µs< 10 µs
Switching response time (electro-optic)Not available (Phase 0)< 1 ns
Phase drift rate< 5 mrad/min< 2 mrad/min
Phase precision (non-volatile elements)Not available (Phase 0)Multi-level; > 5 bits effective
ParameterTargetNotes
Splitting ratio accuracy±1% of 50:50Validates lithographic process
Extinction ratio> 25 dB (Phase 0)Required for MZI interference quality
Insertion loss per element< 1 mdBPer 50:50 split
Fabrication variationCharacterised via test structuresDetermines calibration requirements
ParameterPhase 0 targetPhase 1 target
Insertion loss per facet< 2 dB< 0.1 dB
Polarisation selectivity> 20 dB TM suppression> 30 dB
Wavelength range1530–1570 nm1530–1570 nm
Fibre array pitch127 µm127 µm (standard V-groove)

The Hong-Ou-Mandel (HOM) visibility test measures how indistinguishable two photons are — a critical parameter for quantum gate fidelity. Two photons that are perfectly indistinguishable always bunch together at a 50:50 beam splitter; distinguishable photons do not.

PhaseHOM Visibility TargetSignificance
Phase 0> 90%Minimum for useful quantum operations
Phase 1> 99%Required for fault-tolerant applications

HOM visibility below threshold means photons are too distinguishable to produce reliable quantum entanglement — making the quantum logic unreliable.

For photonic quantum gates (fusion operations):

Gate typeExpected success probabilityFidelity (conditional on success)
Type-I fusion25%> 99% (limited by photon indistinguishability)
Type-II fusion50%> 98%
Single-qubit rotation (MZI)100% (deterministic)> 99.9% (limited by phase precision)

The probabilistic nature of two-photon fusion operations requires running multiple parallel copies of each operation and routing successful outcomes — implemented in the Phase 1+ architecture.

The feed-forward path — detector measurement to correction applied at a downstream element — is critical for measurement-based quantum computation:

ComponentLatency target
Photon detection and amplification~1 ns
ADC digitisation~2 ns
FPGA logic (correction compute)~5 ns
DAC output and element response (electro-optic)~1 ns
Total feed-forward loop~10 ns

A 10 ns feed-forward loop is sufficient for photonic quantum computing where photons travel at approximately 2 × 10⁸ m/s in the waveguide — the correction can be applied before the photon reaches the next stage if the optical path length exceeds approximately 2 m equivalent.

Optical Matrix-Vector Multiplication Latency

Section titled “Optical Matrix-Vector Multiplication Latency”

The computation time for optical matrix multiplication is set by photon propagation time across the chip plus detector readout:

Matrix DimensionOptical transit timeTotal latency (incl. detector)Memory-bound GPU (approx.)
4 × 4< 1 ns~10 ns~10–100 ns
64 × 64< 5 ns~15 ns~100 ns–10 µs
256 × 256< 20 ns~30 ns~1–100 µs
OperationPhotonic platformGPU (approx.)Advantage
64×64 MVM (inference, fixed weights)~1–10 nJ~100–1000 nJ10–100×
256×256 MVM (inference, fixed weights)~5–50 nJ~1–100 µJ20–2000×

Note: The photonic advantage is largest when the same weight matrix is used many times. For single operations or rapidly-changing weights, the reprogramming overhead reduces the advantage.

For AI inference with fixed weights:

ScenarioContinuous phase control powerNon-volatile optical memory powerSaving
64-element network~1 W0 W1 W
256-element network~4 W0 W4 W
1024-element network~15 W0 W15 W

This saving is structural — the weights are stored physically in the material state and require no power to maintain.

Phase 0 uses an external fibre-coupled photon pair source. Typical parameters for the characterisation experiments:

ParameterValueSource
Centre wavelength1550 nmTelecom C-band
Bandwidth~0.3 nm FWHMKTP or PPLN SPDC source
Pair generation rate~MHz at 1 mW pumpTypical for Phase 0 characterisation

On-chip photon pair sources using spontaneous nonlinear optical processes in ring resonators:

ParameterTargetNotes
Pair generation rate> 10 MHz/mW pump powerPublished literature for optimised rings
Photon purity (g²(0))< 0.1Needed for high-visibility quantum interference
Telecom wavelength1550 nm ± 10 nmC-band compatible

Summary: Phase-by-Phase Performance Targets

Section titled “Summary: Phase-by-Phase Performance Targets”
CapabilityPhase 0Phase 1Phase 2
Optical mode count4~64~256
Waveguide loss< 2 dB/cm< 0.5 dB/m< 0.5 dB/m
HOM visibility> 90%> 99%> 99%
Feed-forward latencyNot implemented< 10 ns< 10 ns
Max matrix dimension (AI)4×464×64256×256
Non-volatile optical memoryNot includedIncludedIncluded
On-chip photon sourceNo (external)YesYes