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Single-spin (Loss–DiVincenzo) / nuclear-spin encoding enc_spin_ld

One qubit per spin-1/2 — a confined electron, hole or nucleus — with no encoded subspace, giving the smallest footprint and no leakage channel.

Single-spin (Loss–DiVincenzo) / nuclear-spin encoding

enc_spin_ld · layer 2 Encoding · demonstrated · since 1998

Bare spin-1/2 of an electron, hole or nucleus; needs microwave/EDSR for 1Q.

Brief →

Key references

[819] D. Loss and D. P. DiVincenzo, “Quantum computation with quantum dots,” Phys. Rev. A, vol. … · 1998
[820] F. K. Unseld et al., “Baseband control of single-electron silicon spin qubits in two dimen… · 2025
[189] P. Steinacker et al., “Industry-compatible silicon spin-qubit unit cells exceeding 99% fid… · 2025
[192] H. Edlbauer et al., “An 11-qubit atom processor in silicon,” Nature, vol. 648, no. 8094, p… · 2025

Design space — attributes

(a) carrier affinity
hybrid (fabricated host)
(b) time · entangling
—
(c) readout
—
(d) mobility
—
(e) control
—
(f) error structure
coherent / calibration, stochastic Pauli
(g) manufacturing
—

Evaluation space — dated attributes

no dated attribute

Used by 14 machines (14 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: Atomic-force microscopy images of the two germanium 2×4 quantum dot devices used in this work. Spins are schematically depicted to highlig…
(a, b) Greyscale atomic-force-microscope images of two germanium quantum-dot devices, each a 2×4 grid of dots (200 nm bars), with spins drawn on top: in (a) one spin per dot, 1–8; in (b) dot pairs Q1–Q4 as two-spin (singlet-triplet) qubits. (c) A digital-analog sequence: ramped preparation, microwave drive, SWAP gates, analog evolution of a four-spin plaquette, pairwise measurement; (d–g) double-well cartoons of initialization, readout, drive and a two-spin gate. It is Figure 1 of arXiv 2506.08663, 'Site-resolved magnon and triplon dynamics on a programmable quantum dot spin ladder' (Pablo Cova Fariña, Daniel Jirovec, Menno Veldhorst and co-authors). It shows spin qubits run as a programmable analog simulator. “Fig. 1 — Figure 1: Atomic-force microscopy images of the two germanium 2×4 quantum dot devices used in this work. Spins are schematically depicted to highlight…” by Pablo Cova Fariña et al., arxiv.org/abs/2506.08663, CC BY 4.0 (creativecommons.org/licenses/by/4.0/)
Fig. 2 — Figure 2: Protocol of quantum processing. (a) Circuit for the control protocol includes qubit initialization, operation, and readout. Detailed seque…
Circuit drawings and a plot for two donor clusters in silicon, each with an electron and nuclear spins. (a) Protocol of initialisation, operation and repeated readout; (b) with exchange off, a 2π electron rotation conditioned on its own cluster's nuclear spins; (c) with exchange on, conditioned on spins in both clusters; (d) shift of the electron's spin-resonance frequency versus exchange coupling J from 0 to 200 MHz per nuclear-spin configuration. From 'Scalable Spin Qubit Architecture with Donor-Cluster Arrays in Silicon' (arXiv 2509.24749) by Shihang Zhang et al. Nuclear spins are controlled and read through the electron; exchange makes its resonance depend on both clusters, the basis for a two-cluster gate. “Fig. 2 — Figure 2: Protocol of quantum processing. (a) Circuit for the control protocol includes qubit initialization, operation, and readout. Detailed sequences for…” by Shihang Zhang et al., arxiv.org/abs/2509.24749, CC BY 4.0 (creativecommons.org/licenses/by/4.0/)
Fig. 2 — Figure S1: Nuclear spin flip probabilities during the readout and resonant tunneling pulses. a) Electron tunneling in a 1P1e qubit during the readou…
A six-panel theory figure: energy-level diagrams of a phosphorus donor's combined nuclear and electron spin states, and computed plots of nuclear-spin flip probability over 1 ms. It is Figure S1 of the arXiv paper "Impact of measurement backaction on nuclear spin qubits in silicon" by S. Monir and co-authors, including M.Y. Simmons and R. Rahman. It illustrates spin-to-charge readout of a donor, where the electron tunnels to a single-electron transistor: notice that the flip probabilities during readout and resonant-tunnelling pulses stay tiny, around 10^-6 to 10^-5. “Fig. 2 — Figure S1: Nuclear spin flip probabilities during the readout and resonant tunneling pulses. a) Electron tunneling in a 1P1e qubit during the readout pulse.…” by S. Monir et al., arxiv.org/abs/2310.12656, CC BY 4.0 (creativecommons.org/licenses/by/4.0/)
enc_spin_ld · layer 2 Encoding · centrality 5.5 · demonstrated · since 1998 · updated 2026-09-30

Single-spin (Loss–DiVincenzo) / nuclear-spin encoding

One qubit per spin-1/2 — a confined electron, hole or nucleus — with no encoded subspace, giving the smallest footprint and no leakage channel.

Verdict. The default encoding on every silicon, germanium, donor and defect platform; it buys minimum area and a clean Pauli error model at the cost of a resonant drive per qubit.

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

One physical spin-1/2 is one qubit: an electron or hole in a gate-defined dot, or a nucleus bound to a donor or defect. Loss and DiVincenzo set it out in 1998 — dot-confined electron spins, rotations by a local resonant field, two-qubit gates by pulsed exchange D[819]. The nuclear variant drives a ³¹P or defect nucleus by radio frequency through hyperfine coupling to an electron, trading speed for coherence: nuclei as data, electrons as ancillas. Attributes: affinity — a near-natural carrier with no composite structure; error — coherent dephasing plus Pauli error, no leakage subspace, no control modality or fabrication of its own.

Physics & limits

The computational space is the whole two-level system: nothing leaks out, so every error is Pauli or coherent as the codes assume — and nothing is filtered out either. T2* is set by residual ²⁹Si hyperfine coupling and by charge noise turned into a frequency shift through the g-factor or a micromagnet; ²⁸Si purification removes the first term. Coherence is not the limit today: QuTech's microwave-free array bounds its hopping gate at ≥99.50(6)% D[820] and foundry two-qubit gates sit at 99.04–99.56% D[189] — a calibration-limited plateau, not a T2 limit. Deeper purification, baseband control and cold calibration move the floor.

Engineering state of the art

table
year figure who tag+key
2025-07-01 ≥99.50(6)% hopping gate (lower bound), no microwave, 2×2 array QuTech/TU Delft D[820]
2025-09-24 99.04–99.56% two-qubit on 300 mm foundry SiMOS Diraq D[189]
2025-12-17 11-qubit donor register, 9 nuclear plus 2 electron, 99.10–99.99% Silicon Quantum Computing D[192]

Dominant term: calibration drift across the array; no device above 12 qubits publishes all-pairs fidelities.

The 99.90% donor nuclear-spin CZ fidelity cannot be isolated in the SQC abstract, whose published range is 99.10–99.99%. Intel's "scale to hundreds of dots" carries no date or milestone.

Manufacturing, materials & supply chain

The encoding adds no structure — one dot or donor per qubit, about a third of the dots an exchange-only qubit needs — and inherits the carrier's process: Intel's 300 mm EUV line at >24,000 devices per wafer D[199] and 96% tune-up yield on 232 devices of one wafer D[766], plus 22FDX, FD-SOI and imec 300 mm. The burden it imposes is control: one resonant drive per qubit frequency, so at 10³ qubits the wall is frequency crowding and microwave power at millikelvin, at 10⁴–10⁶ the count of addressable tones.

Role in the stack

The base encoding for the silicon and germanium quantum-dot architecture, the donor architecture and defect-spin network nodes. It is replaced in some designs by exchange-only encoding — the central fork: microwave hardware for minimum footprint and no leakage, against extra dots for baseband-only control and a leakage channel. It adds nothing to derived clock = sum of the syndrome round: gate layers + transport + readout + reset, which on silicon stays readout-dominated at 8.5×10⁻⁶ s. Verification: the 99.50(6)% is a lower bound and the accompanying ~49 µs Hahn-echo a maximum, both routinely requoted as point estimates D[820]; the main report's "99.90% donor nuclear CZ" conflicts with the published SQC range D[192]; and HRL's 2×10⁻⁴ single-qubit error belongs to exchange-only encoding, not this one D[190].

Actors & economics

Who.
| Organisation | Role | Country | What they do | Evidence |
|---|---|---|---|---|
| Intel | developer | USA | 300 mm EUV single-spin devices | D[199] |
| Diraq | developer | Australia | Electron spins on 300 mm imec SiMOS | D[189] |
| QuTech/TU Delft | research | Netherlands | Microwave-free baseband control | D[820] |
| Silicon Quantum Computing | developer | Australia | Nuclear-spin encoding on donors | D[192] |
| Quobly | developer | France | Single spins on STMicroelectronics FD-SOI | Cfact |

Money. 2026-06-03 · Quobly · Series A · €115 M · Bpifrance, SEALSQ, STMicroelectronics · €134 M cumulative · closed Cfact. 2026-06 · SQC · NRFC · A$60 M · Australia's National Reconstruction Fund · closed fact.

Market & supply chain. No supplier is specific to this encoding — it is a layout and pulse-sequence choice on shared CMOS lines — and its one distinctive demand, a resonant drive per qubit, is what the control-electronics duopoly sells. Pays into G2, G3 and G6.

IP & standards. The 1998 proposal is prior art long out of patent term D[819]; no dated patent family for single-spin encoding found in a named database as of 4 Sep 2026.

Roadmaps & track record. Intel (2026-01-06 · 12 qubits at Argonne, "scale to hundreds of dots" · no successor chip, no dated roadmap) fact. Diraq (2026-08-27 · 150 k physical, 1 k logical by 2029 · its 2026-07-09 release said "thousands by 2029") Rfact. Both are orders of magnitude beyond any demonstrated device.

Strategic reading. Every spin team can fall back on it, so it differentiates nobody: value accrues to the fab and the control stack. If baseband control matures the microwave vendors lose their strongest claim; if encoded qubits win, area matters less than wafer economics.

Outlook & open questions

Confirm or demote in 12–24 months: all-pairs fidelities above 12 qubits; baseband control beyond a 2×2 array. Best case 2029: baseband plus 1 K operation removes most microwave I/O at >99.5% two-qubit fidelity. Worst case: the plateau holds. Open: (1) whether hopping-gate control scales past four qubits; (2) whether the calibration-limited diagnosis generalises; (3) which platform shows a below-threshold logical qubit.

References
  1. [189] P. Steinacker et al., “Industry-compatible silicon spin-qubit unit cells exceeding 99% fidelity,” Nature, vol. 646, no. 8083, pp. 81–87, Sep. 2025, doi: 10.1038/s41586-025-09531-9. D
  2. [190] Members of the HRL Quantum Team and Collaborators, “A digitally controlled silicon quantum processing unit,” arXiv:2604.16216, Apr. 2026. D
  3. [192] H. Edlbauer et al., “An 11-qubit atom processor in silicon,” Nature, vol. 648, no. 8094, pp. 569–575, Dec. 2025, doi: 10.1038/s41586-025-09827-w. arXiv:2506.03567. D
  4. [199] H. C. George et al., “12-spin-qubit arrays fabricated on a 300 mm semiconductor manufacturing line,” Nano Lett., vol. 25, no. 2, pp. 793–799, Dec. 2024, doi: 10.1021/acs.nanolett.4c05205. arXiv:2410.16583. D
  5. [766] S. F. Neyens et al., “Probing single electrons across 300-mm spin qubit wafers,” Nature, vol. 629, no. 8010, pp. 80–85, May 2024, doi: 10.1038/s41586-024-07275-6. D
  6. [819] D. Loss and D. P. DiVincenzo, “Quantum computation with quantum dots,” Phys. Rev. A, vol. 57, no. 1, pp. 120–126, Jan. 1998, doi: 10.1103/PhysRevA.57.120. D
  7. [820] F. K. Unseld et al., “Baseband control of single-electron silicon spin qubits in two dimensions,” Nat. Commun., vol. 16, no. 1, Art. no. 5605, Jul. 2025, doi: 10.1038/s41467-025-60351-x. D