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Linear-optical fusion (heralded) g_fusion

Probabilistic Bell-basis measurement on two photons — 50% unboosted, 75% with ancillae — whose failure is heralded and erases one of the two measured outcomes; the entangling primitive of fusion-based photonics.

Linear-optical fusion (heralded)

g_fusion · layer 3 Gate mechanism · demonstrated · since 2005

Probabilistic Bell measurement on photons (50%, 75% boosted); failure is heralded → erasure.

Brief →

Key references

[451] D. E. Browne and T. Rudolph, “Resource-Efficient Linear Optical Quantum Computation,” Phys… · 2005
[419] F. Ewert and P. van Loock, “3/4-Efficient Bell Measurement with Passive Linear Optics and … · 2014
[169] K. Alexander et al., “A manufacturable platform for photonic quantum computing,” Nature, v… · 2025
[264] M. C. Löbl, L. A. M. Pettersson, J. Dragašević, S. X. Chen, and O. A. D. Sandberg, “The su… · 2026

Design space — attributes

(a) carrier affinity
photon (natural particle, engineered modes)
(b) time · entangling
100 ns · probabilistic / heralded
(c) readout
—
(d) mobility
flying qubits (photons)
(e) control
electro-optic @ room temperature
(f) error structure
loss (erasure)
(g) manufacturing
photonic IC foundry

Evaluation space — dated attributes

fusion Bell fidelity → 99.22%
defines: error channel · 2025-02 · source

Standard records

2Q error under full-width parallel operation → not published · typical
Fusion Bell-state fidelity 99.22(12)% is a single-fusion measurement; no parallel or network-scale fusion figure is published · 2025-02 · source [D] ⓘ
crosstalk → not published · typical
No crosstalk figure: fusion failure is heralded and enters the loss budget, not a coherent-error budget · 2025-02 · source [D] ⓘ

Actors & goals — annotations

Continuous-variable photonic — GKP (alternate) — Xanadu (Aurora) · G4 G6

Used by 6 machines (6 primary · 0 alternate)

↗ its register card · paper / product / press: links that name the machine (attribution checked on 20 Sep 2026)

Pictures

Every picture carries the story of what it shows and its credit line.

Fig. 1 — Figure 1: Comparison between standard and logical Bell-state measurements (BSMs). (a) Schematic representation of the logical BSM. Four physical qub…
A drawing and a table. (a) A logical Bell-state measurement (BSM) built from two standard linear-optical BSMs, each a 50:50 beam splitter followed by half-wave plates, polarising beam splitters and detectors, on four physical qubits a–d. (b) Success probabilities: the standard BSM identifies two of four Bell states (average 50%), the logical BSM two always and two half the time (average 75%). It is Figure 1 of arXiv 2609.10698, 'Demonstration of a logical Bell-state measurement beyond the linear-optical limit', by Shreya Kumar, Simon D. Reiß, Peter van Loock and Stefanie Barz. A plain linear-optical BSM works only half the time; beating that matters for fusion-based photonic quantum computing. “Fig. 1 — Figure 1: Comparison between standard and logical Bell-state measurements (BSMs). (a) Schematic representation of the logical BSM. Four physical qubits encode…” by Shreya Kumar, Simon D. Reiß, Peter van Loock, Stefanie Barz, arxiv.org/abs/2609.10698, CC BY 4.0 (creativecommons.org/licenses/by/4.0/)
Fig. 2 — Figure 2: Experimental implementation of the logical BSM. The setup is primarily composed of two parts: The logical Bell-state generation and the lo…
A rendered drawing of a tabletop photonics experiment: a 775-nanometre picosecond laser pumps two ppKTP crystals that make entangled photon pairs, which travel by fibre to two beam-splitter Bell-state measurements read out by superconducting nanowire detectors. It comes from arXiv paper 2609.10698 by Shreya Kumar, Simon D. Reiß, Peter van Loock and Stefanie Barz. Such Bell-state measurements are the 'fusion' step of photonic quantum computing; notice the dashed line separating state generation from measurement. It is a drawing, not a photograph. “Fig. 2 — Figure 2: Experimental implementation of the logical BSM. The setup is primarily composed of two parts: The logical Bell-state generation and the logical BSM.…” by Shreya Kumar, Simon D. Reiß, Peter van Loock, Stefanie Barz, arxiv.org/abs/2609.10698, CC BY 4.0 (creativecommons.org/licenses/by/4.0/)
Fig. 3 — Figure 3: The most common applications of BSMs in quantum information: a) Entanglement swapping protocol, which allows to share an entangled photon…
A three-panel drawn schematic, not an experiment photograph, from the review "Bell state measurements in quantum optics: a review of recent progress and open challenges" by Luca Bianchi, Carlo Marconi and Davide Bacco. It shows three uses of a Bell state measurement: entanglement swapping between photon pairs, fusion gates that join small photonic graph states into larger cluster states for measurement-based quantum computing, and measurement-device-independent quantum key distribution. Notice that the same measurement box is the core of all three. “Fig. 3 — Figure 3: The most common applications of BSMs in quantum information: a) Entanglement swapping protocol, which allows to share an entangled photon pair…” by Luca Bianchi, Carlo Marconi, Davide Bacco, arxiv.org/abs/2509.18756, CC BY 4.0 (creativecommons.org/licenses/by/4.0/)
g_fusion · layer 3 Gate mechanism · centrality 7.7 · demonstrated · since 2005 · updated 2026-09-03

Linear-optical fusion (heralded)

Probabilistic Bell-basis measurement on two photons — 50% unboosted, 75% with ancillae — whose failure is heralded and erases one of the two measured outcomes; the entangling primitive of fusion-based photonics.

Verdict. Real: single fusions at 99.22% Bell fidelity on chip, 99.72% chip-to-chip (PsiQuantum, 2025-02). Unproven: any chained fusion network with an end-to-end success rate. Demote if no multi-fusion result is published by 2028.

Key references

Λ = error-suppression factor per code-distance step; QBI = DARPA Quantum Benchmarking Initiative (Stage A concept → B R&D plan → C government V&V); G1–G7 = the report's goal classes (see Actors & economics).

Identity & lineage

A Bell-basis measurement — beamsplitter, phase shifters, number-resolving detectors — projecting two photons onto a Bell state or destroying both and saying so, handing the code erasure rather than Pauli error. Browne and Rudolph introduced type-I/II fusion in 2005 to grow cluster states without a deterministic gate S[451]; linear optics caps unambiguous discrimination at 50%, unentangled ancillae lift it to 75% S[419]. Attributes: flying photons, heralded entangling at ~100 ns; electro-optic room-temperature control, loss-dominated errors, photonic-IC fabrication.

Physics & limits

The 50% ceiling is a linear-optics bound (Calsamiglia & Lütkenhaus 2001): passive optics with vacuum ancillae distinguishes at most two of the four Bell states, and the ancilla photons that raise it to 75% and beyond must themselves survive. The operating figure is success probability × transmission²; loss turns a success into heralded failure at best, an undetected error at worst. The gate is not the problem: 99.22 ± 0.12% on chip, 99.72 ± 0.04% chip-to-chip over 42 m at ~2 K D[169]fact. The floor is the path around it — SiN 1.8 ± 0.2 dB/m, BTO switch 100 mdB, fibre-to-chip 52 mdB, on-chip SNSPD 93.4% median D[169] — and failure itself: a 2026 re-analysis puts a logical-error floor at zero loss, so all-linear-optics designs need very large distance, while emitter-mediated fusion tolerates 7.0–7.3% S[264]fact.

Engineering state of the art

table
Date Figure Who Tag
2005 Type-I/II fusion, 50% success, proposed Browne & Rudolph S[451]
2014 75% Bell measurement with unentangled ancillae Ewert & van Loock S[419]
2025-02 Bell fidelity 99.22 ± 0.12% on chip; 99.72 ± 0.04% chip-to-chip, 42 m PsiQuantum D[169]
2026-06 Fusion-failure noise floor at zero loss; 7.0–7.3% threshold Sparrow S[264]

Every dated fidelity is one fusion measured alone; no chained-fusion success rate is public.

No second group has replicated PsiQuantum's 99.22%/99.72% fusion fidelities as of 4 Sep 2026. Quandela's Lucy is described by its sources only as a 12-photonic-qubit machine, not as a fusion-based system. The main report's PsiQuantum waveguide loss of 0.5 dB/m conflicts with the Nature paper's 1.8 ± 0.2 dB/m for single-mode SiN, the figure used here.

Manufacturing, materials & supply chain

No fusion-specific materials: the gate reuses the platform stack — SiN waveguides, BTO switches, on-chip SNSPDs on 300 mm silicon at GlobalFoundries Cfact. Manufacturing decides loss per element, and every element sits inside the attempt: switch 100 mdB, fibre-to-chip 52 mdB D[169]; best packaged coupling is Xanadu's 0.085 dB/facet Cfact. I/O is channels and latency: 2–4 number-resolving detectors per fusion plus feed-forward within the photon's flight time; Aurora runs 12 modes on a 1 MHz cycle D[173]. At 10³ fusions/s the constraint is accumulated switch loss; at 10⁴–10⁶, cryogenic channel count and GHz feed-forward, unbuilt. ECCN 4A906 covers the machine, 3A901 sub-4.5 K electronics fact.

Role in the stack

Requires single photons, single-photon detection for heralding and electro-optic switching for feed-forward; provides the fusion measurements consumed by resource-state generation and fusion-based fault tolerance (PsiQuantum, Quandela, QuiX). It replaces CV Gaussian combination on the continuous-variable photonic GKP architecture (Xanadu), where it is an alternate — switching changes detectors, encoding and error model together. Clock contribution ~1.0 × 10⁻⁷ s per attempt, divided by success probability and multiplexing depth, so generation, not the gate, dominates the derived clock. Verification: the headline numbers are tomography of one fusion; no protocol reports success-at-depth, and no second group has replicated them.

Actors & economics

Who.
Organisation Role Country What they do Evidence
PsiQuantum developer US Highest published fusion fidelity, 300 mm line Dfact
Quandela developer FR Fielded linear-optical hardware Cfact
QuiX Quantum developer NL MBQC hardware at DLR Cfact
Sparrow Quantum research DK Threshold case against linear-optics fusion Sfact
DARPA investor US Funds PsiQuantum Stage C, Quandela QBIT fact

Money.
2025-09-10 · PsiQuantum · Series E · USD 1 B at USD 7 B · BlackRock, Temasek · closed fact
2026-06-16 · Quandela · DARPA QBIT Stage A · undisclosed · announced fact
2026-07-22 · PsiQuantum · DARPA QBI Stage C expansion · USD 125 M · definitive fact

Market & supply chain. No separate market: fusion ships inside a photonic IC, so the foundry and packaging house set its usable success probability. Concentration risk sits with GlobalFoundries; only G3/G4 pay.

IP & standards. No dated patent family specific to the fusion gate as of 4 Sep 2026; nearest is ORCA's US 12,437,225 fact.

Roadmaps & track record. (2025-02 · Omega component metrics · delivered); (2026-07 · Stage C V&V of switches, packaging, cryogenics · in progress, funding validation not publication). Component credibility good, system-level fusion untested.

Strategic reading. Component fidelity is table stakes; the contest is success rate at depth, where the 2026 threshold argument favours emitter-mediated fusion — a challenge to PsiQuantum and QuiX, an opening for quantum-dot vendors. If linear optics holds, foundries capture the value.

Outlook & open questions

Confirm by 2027: a published network of ≥3 chained fusions with end-to-end success rate and erasure statistics; demote if only single-fusion figures exist by 2028. Best case 2029: boosted fusion above 75% on chip. Worst case: the zero-loss failure floor holds and linear-optical fusion survives only inside emitter hybrids. Open: how correlated failures are across a chip; whether 93%-efficient number resolution supports boosting.

References
  1. [169] K. Alexander et al., “A manufacturable platform for photonic quantum computing,” Nature, vol. 641, no. 8064, pp. 876–883, Feb. 2025, doi: 10.1038/s41586-025-08820-7. D
  2. [173] H. A. Rad et al., “Scaling and networking a modular photonic quantum computer,” Nature, vol. 638, no. 8052, pp. 912–919, Jan. 2025, doi: 10.1038/s41586-024-08406-9. D
  3. [264] M. C. Löbl, L. A. M. Pettersson, J. Dragašević, S. X. Chen, and O. A. D. Sandberg, “The subthreshold issue of fusion-based quantum computing,” arXiv:2606.28490, Jun. 2026. S
  4. [419] F. Ewert and P. van Loock, “3/4-Efficient Bell Measurement with Passive Linear Optics and Unentangled Ancillae,” Phys. Rev. Lett., vol. 113, no. 14, Art. no. 140403, Sep. 2014, doi: 10.1103/PhysRevLett.113.140403. arXiv:1403.4841. S
  5. [451] D. E. Browne and T. Rudolph, “Resource-Efficient Linear Optical Quantum Computation,” Phys. Rev. Lett., vol. 95, no. 1, Art. no. 010501, Jun. 2005, doi: 10.1103/PhysRevLett.95.010501. S