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Spin–photon solid-state link (SiV, NV, T centre) ic_spinphoton

Heralded photonic entanglement between separated solid-state spin registers — diamond NV and SiV centres, silicon T centres — through deployed telecom fibre.

Spin–photon solid-state link (SiV, NV, T centre)

ic_spinphoton · layer 9 Interconnect · demonstrated · since 2013

Entanglement over 25–35 km deployed fibre at 0.02–1 Hz with F 0.53–0.86; two distinct inter-cryostat teleported-CNOT results — post-selected on T centres (Photonic Inc.) and unconditional on NV (QuTech).

Reading marks
crossing technology — fabricated/solid-state carrier + photonic interconnect
Brief →

Key references

[783] H. Bernien et al., “Heralded entanglement between solid-state qubits separated by three me… · 2013
[784] A. J. Stolk et al., “Metropolitan-scale heralded entanglement of solid-state qubits,” Sci.… · 2024
[209] C. M. Knaut et al., “Entanglement of nanophotonic quantum memory nodes in a telecom networ… · 2024
[363] F. Afzal et al., “Distributed Quantum Computing in Silicon,” arXiv:2406.01704, Jun. 2024. · 2024

Design space — attributes

(a) carrier affinity
intermediate / carrier-agnostic
(b) time · entangling
—
(c) readout
—
(d) mobility
flying qubits (photons)
(e) control
optical @ room temperature
(f) error structure
loss (erasure)
(g) manufacturing
diamond growth / implantation

Evaluation space — dated attributes

SiV over 35 km → F = 0.69, ≤ 1 Hz
defines: error channel · 2024-05 · source
NV Delft–The Hague 25 km → F = 0.534, 0.022 s⁻¹
defines: error channel · 2024-04 · source
T-centre inter-cryostat link (Photonic Inc.) → Bell F = 0.60(8) at 7.5 mHz; teleported-CNOT sequence post-selected, no gate fidelity
defines: error channel · 2024-06 · source
NV unconditional teleported CNOT (QuTech) → 63(4)% (4-qubit GHZ 64(4)%), real-time feed-forward, no post-selection
defines: error channel · 2026-05 · source

Both results exist and differ in kind: Photonic Inc.'s 2024 T-centre demonstration is a post-selected preprint with a truth table rather than a gate fidelity; QuTech's 2026 NV result is unconditional. Quoting them together without that distinction overstates the T-centre platform.

Edges

needs: Colour-centre / defect spin (NV, SiV, SnV, T centre), Single-photon detection (SNSPD / TES)
needed by: Non-local qLDPC codes (bivariate bicycle, 'gross')°
° one of several that would do · the usual route, not a strict need

Used by 1 machine (1 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. 2 — Figure 2: Photonic crystal integration with a SiN optical waveguide. (a) SEM image of an integrated diamond photonic crystal on an optical waveguide…
An eight-panel figure. (a) A false-coloured scanning electron micrograph (5 µm scale bar) of a diamond photonic-crystal nanobeam (cyan, row of holes) laid across a silicon-nitride (SiN) waveguide taper (yellow) between aluminium pads, with a drawn layer-stack cross-section and an optical image of the chip edge (1 mm); (b), (e), (f) draw the diamond-to-SiN taper and the SiN-to-fibre edge coupler; (c), (d), (g), (h) plot their transmission against misalignment, taper length and top-layer refractive index. It comes from arXiv 2604.06984 by H. Kurokawa, H. Kosaka and co-authors. It shows how light from diamond colour-centre cavities reaches optical fibre for spin–photon links; the fibre is drawn, not photographed. “Fig. 2 — Figure 2: Photonic crystal integration with a SiN optical waveguide. (a) SEM image of an integrated diamond photonic crystal on an optical waveguide chip. The…” by H. Kurokawa et al., arxiv.org/abs/2604.06984, CC BY 4.0 (creativecommons.org/licenses/by/4.0/)
Fig. 3 — Figure 4: Nuclear spin entanglement distribution through 35 km of deployed fiber. a. Schematic of quantum frequency conversion setup. At node A, the…
A four-panel figure (captioned Figure 4): (a) a drawing of two nodes built on silicon-vacancy centres in nanophotonic cavities, linked by converters that shift 737 nm photons to 1350 nm for telecom fibre; (b)–(c) plots of entanglement fidelity versus fibre length and of two-qubit measurement outcomes; (d) a street map of Boston/Cambridge tracing a 35 km deployed fibre loop. It comes from "Entanglement of Nanophotonic Quantum Memory Nodes in a Telecom Network" by Knaut, Suleymanzade, Wei and co-authors. Notice nuclear-spin entanglement fidelity staying above the dashed classical bound of 0.5. “Fig. 3 — Figure 4: Nuclear spin entanglement distribution through 35 km of deployed fiber. a. Schematic of quantum frequency conversion setup. At node A, the photonic…” by Can M. Knaut et al., arxiv.org/abs/2310.01316v2, CC BY 4.0 (creativecommons.org/licenses/by/4.0/)
Fig. 2 — Figure 2: Large-scale device integration. Optical images of (A) the 2-mm diamond chip and (B) a close up of one of the 16 sets of devices. Thru/drop…
A seven-panel paper figure: optical images of a 2-mm diamond chip carrying 16 sets of gallium phosphide resonators, electron micrographs of single devices, and room-temperature spectra and quality-factor data for 321 devices. It is Figure 2 of arXiv 2601.04733 by Nicholas S. Yama, Chun-Chi Wu, Fariba Hatami and Kai-Mei C. Fu. It shows how optical cavities for spin-photon interfaces can be made in large numbers on diamond; note the spread of resonance wavelengths and the grey band of devices that can be tuned onto the emitter. “Fig. 2 — Figure 2: Large-scale device integration. Optical images of (A) the 2-mm diamond chip and (B) a close up of one of the 16 sets of devices. Thru/drop devices…” by Nicholas S. Yama, Chun-Chi Wu, Fariba Hatami, Kai-Mei C. Fu, arxiv.org/abs/2601.04733, CC BY 4.0 (creativecommons.org/licenses/by/4.0/)
ic_spinphoton · layer 9 Interconnect · centrality 10.4 · demonstrated · since 2013 · updated 2026-09-30

Spin–photon solid-state link (SiV, NV, T centre)

Heralded photonic entanglement between separated solid-state spin registers — diamond NV and SiV centres, silicon T centres — through deployed telecom fibre.

Verdict. Inter-cryostat gates exist on both hosts, unconditionally on NV (63–64%) and only post-selected on T centres. Rates of 0.0075–1 Hz sit 10⁵–10⁷ below the ~200 kHz reported as Photonic Inc.'s architecture target, an unverified figure; loss, not coherence, is why.

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

Each node is a spin qubit in a solid — a nitrogen-vacancy or silicon-vacancy centre in diamond, or a silicon T centre — whose optical transition emits a photon entangled with the spin. Photons from two nodes interfere on a beamsplitter; a detection pattern heralds spin–spin entanglement without trusting the channel, so loss costs attempts, not fidelity. Delft demonstrated the first heralded solid-state version across 3 m in 2013 D[783]; everything since has pushed that protocol into deployed telecom fibre.

  • Mobility: the carrier flies (a photon in fibre); both spins stay fixed.
  • Error structure: loss-dominated; conditional fidelity and unconditional rate must be quoted together.

Physics & limits

The floor is the product of collection, conversion and transmission efficiencies, entering the rate quadratically for two-photon protocols and linearly for the single-photon protocol Delft uses at metropolitan scale D[784]. The coherent zero-phonon line carries ~3% of an NV centre's emission, ~23% of a T centre's and 65–90% of an SiV's Dfact, and a 35 km deployed urban loop costs a further 17 dB D[209]. Wavelength decides whether conversion is needed — NV at 637 nm and SiV at 737.2 nm require it (Harvard converts to 1,350 nm), while a T centre emits natively near 1,326 nm, skipping that stage but paying with a weaker transition P[363]. Spin coherence is not the constraint: nuclear memories hold entanglement beyond 2 s D[209], far longer than the 0.25–0.35 ms fibre round trip. The one lever that moves the floor is cavity enhancement — a fibre microcavity around one NV raised resonant collection roughly tenfold, ~0.05% to ~0.5%, keeping echo coherence above 100 µs D[359]; one more such step would pass the ~2% per-attempt photon success that 0.8-NA objectives give a trapped ion D[116].

Engineering state of the art

table
Year Figure Who Tag+key
2024-04 NV, nodes 10 km apart over 25 km deployed fibre with telecom L-band conversion: F = 0.534 at 0.022 s⁻¹ QuTech/Delft D[784]
2024-05 SiV: F = 0.69(7) between nuclear memories over a 35 km deployed Boston loop; 0.86(3) electron–electron at 20 m, ≤1 Hz Harvard D[209]
2024-06 T centre, two modules in separate cryostats over ~40 m fibre: Bell F = 0.60(8), ~7.5 mHz; teleported-CNOT sequence post-selected, no gate fidelity Photonic Inc. P[363]
2026-05 Unconditional teleported CNOT between NV registers in separate cryostats: 4-qubit GHZ 64(4)%, CNOT-mediated state 63(4)% QuTech/Delft Dfact

The dominant term is collection and heralding efficiency, not spin coherence or in-node gate error.

Manufacturing, materials & supply chain

Diamond nodes need quantum-grade CVD material, for which Element Six (UK) is the reference supplier Pfact, plus nanophotonic cavities whose yield is the blocker and is unpublished: a 2026 Delft tin-vacancy study characterised 327 cavities on two chips at room temperature, found coupled centres in 7 of the 9 it cooled and measured two above cooperativity one Dfact — no chip-wide fraction, the number any 10²-node proposal needs. Silicon T centres trade emitter quality for process maturity: implantation into enriched ²⁸Si on a CMOS line, with the centres operated at ~1.5–4 K, not millikelvin P[785]. Both ends depend on nanowire detectors from a five-vendor merchant base — Single Quantum, ID Quantique (owned by IonQ), Photon Spot, Quantum Opus and Moscow's Scontel Pfact. No export-control classification names spin–photon links.

Control, readout & I/O burden

Per node: a cryostat, microwave spin control, resonant lasers for initialisation and readout, a conversion stage unless the emitter is already telecom, phase-stabilised fibre to the midpoint, and detectors. The binding burden is duty cycle, not latency: at 0.022 s⁻¹ one link spends 45 s per Bell pair while stabilisation loops run continuously. Ten nodes are an experiment; 10² at sub-Hz cannot serve a distributed processor, and 10³ needs multiplexed emitters and detector arrays nobody has fielded.

Role in the stack

It requires a colour-centre spin register and single-photon detection; without low-dark-count detectors heralding fails outright. It provides for nothing further and tops the defect-spin network architecture. On any distributed architecture it is the pacing term: no code runs on the defect architecture, so in place of a sum of the syndrome round: gate layers + transport + readout + reset the clock is 45 s at Delft's metropolitan rate and 1.0 s at Harvard's best. The comparison that matters is the competing interconnect: Oxford's trapped-ion link reached 96.89(8)% Bell fidelity at 9.7 s⁻¹ with an 86.2(9)% teleported CZ Dfact — against Harvard's best SiV link, 0.86(3) at up to 1 Hz over 20 m, about ten times the rate and 11 points higher, and its teleported gate 23 points above QuTech's unconditional 63(4)% D[209]Dfact. Solid-state's counter-argument is manufacturability, not performance.

Evidence — how the numbers were measured

The teleported-CNOT attribution resolves, and not as a mis-attribution: both results exist and differ in kind. Photonic Inc. entangled two T-centre modules in separate cryostats over ~40 m and ran a teleported-CNOT sequence, but forwent feed-forward and post-selected on a photon detection, reporting a truth table rather than a gate fidelity; still a 2024 preprint as of 4 Sep 2026 P[363]. QuTech's 2026 result is unconditional — real-time feed-forward, no post-selection — at 63(4)% and 64(4)% Dfact. Quoting the two together without that distinction overstates the T-centre platform. Elsewhere fidelities are conditional on a herald, and Harvard rejects ~23% of data on reflectance-contrast thresholds D[209]. No result here has a second-group replication.

Not published: a dated patent-family count for spin–photon links.

Actors & economics

Who.
| Organisation | Role | Country | What exactly they do | Evidence |
|---|---|---|---|---|
| QuTech | Research | Netherlands | Metropolitan NV link; the only unconditional inter-cryostat gate | Dfact |
| Photonic Inc. | Developer | Canada | Silicon T-centre modules, native telecom emission | P[363] |
| Harvard University | Research | USA | SiV nanophotonic nodes over a 35 km deployed loop | D[209] |
| Fujitsu | Funder | Japan | Funds the Delft modular-computer joint programme | Pfact |
| Microsoft | Investor, partner | USA | Networking collaboration since 2023; returning investor | Cfact |
| Single Quantum | Supplier | Netherlands | Merchant nanowire detectors, the heralding dependency | Pfact |

Money. 2025-11-06 · Photonic Inc. · DARPA QBI Stage B, ~12 months · up to $15 M USD · programme fact. 2026-05-12 · Photonic Inc. · final close · $200 M USD at $2 B valuation, $350 M cumulative · Microsoft returning · closed Cfact. Ongoing · QuTech · Fujitsu joint programme PPS2007, EU Quantum Internet Alliance grant 101080128, NWO Spinoza · not itemised · ongoing Pfact.

Market & supply chain. No one sells a spin–photon link; the sold goods are detectors, diamond, enriched ²⁸Si, conversion modules and leased metro fibre. Detector supply is the shared bottleneck — five merchant vendors, one now owned by IonQ — and diamond comes mostly from one supplier, Element Six. It pays for G6 by definition and G7 where a modular machine needs inter-module links; not for G1–G5, which is why its money is programme funding — DARPA QBI, the Fujitsu–Delft joint programme, the EU Quantum Internet Alliance, NWO — plus one venture-backed developer, Photonic Inc.

IP & standards. No patent family specific to spin–photon links was located in a named dated database as of 4 Sep 2026; Photonic Inc.'s T-centre position originates in Simon Fraser University work, but no assignee-and-date record was retrieved. No standards body governs heralding interfaces; the EU Quantum Internet Alliance is the nearest coordinating structure.

Roadmaps & track record. Photonic Inc. (promised 2023 · distributed fault tolerance "within five years", ~2028 · status 4 Sep 2026: no multi-node system, the 2024 link still post-selected), with a target of ~200 kHz at 99.8% R[785] — seven orders of magnitude in rate and 40 points above its own published result, so an architecture target, not a roadmap. QuTech publishes no roadmap and delivers a Nature-class result roughly annually — credible on delivery, honest about rates.

Strategic reading. If this link matures the winners are modular architectures that cannot scale monolithically, and Microsoft gains optionality on a layer it need not build. Losers are monolithic roadmaps assuming on-chip scaling suffices. The substitution threat is ahead on points: trapped-ion links are faster and cleaner, and microwave-to-optical transduction targets the same slot. Bargaining power sits with detector and diamond suppliers.

Outlook & open questions

Confirm by 2028 if any group sustains > 1 Hz heralded entanglement above F = 0.8 over > 20 km of deployed fibre, or if Photonic Inc. publishes an unconditional inter-module gate with a fidelity; demote if T-centre results stay post-selected preprints. Best case 2029: cavity enhancement plus multiplexing reaches 10–100 Hz at metropolitan distance. Worst case: sub-Hz rates, fidelity near 0.7, ion-photon links taking the slot. Open questions: does native telecom emission beat conversion once T-centre photon yield is counted; what fraction of a chip's cavities exceeds cooperativity one, and can it reach what a 100-node network needs; does anyone multiplex across emitters.

References
  1. [116] J. O'Reilly et al., “Fast photon-mediated entanglement of continuously-cooled trapped ions for quantum networking,” Phys. Rev. Lett., vol. 133, Art. no. 090802, Aug. 2024, doi: 10.1103/PhysRevLett.133.090802. arXiv:2404.16167. D
  2. [209] C. M. Knaut et al., “Entanglement of nanophotonic quantum memory nodes in a telecom network,” Nature, vol. 629, no. 8012, pp. 573–578, May 2024, doi: 10.1038/s41586-024-07252-z. D
  3. [359] J. Fischer et al., “Spin-photon correlations from a Purcell-enhanced diamond nitrogen-vacancy center coupled to an open microcavity,” Nat. Commun., vol. 16, no. 1, Art. no. 11680, Nov. 2025, doi: 10.1038/s41467-025-66722-8. D
  4. [363] F. Afzal et al., “Distributed Quantum Computing in Silicon,” arXiv:2406.01704, Jun. 2024. P
  5. [783] H. Bernien et al., “Heralded entanglement between solid-state qubits separated by three metres,” Nature, vol. 497, no. 7447, pp. 86–90, May 2013, doi: 10.1038/nature12016. D
  6. [784] A. J. Stolk et al., “Metropolitan-scale heralded entanglement of solid-state qubits,” Sci. Adv., vol. 10, no. 44, Art. no. eadp6442, Oct. 2024, doi: 10.1126/sciadv.adp6442. arXiv:2404.03723. D
  7. [785] M. Ivezic, “Photonic Inc,” PostQuantum.com, Nov. 13, 2025. [Online]. Available: https://postquantum.com/quantum-computing-companies/photonic-inc/ P