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Hyperfine / clock-state qubit enc_hf

Two ground-state hyperfine or nuclear-spin sublevels at a field-insensitive clock point, the default qubit for every trapped-ion and neutral-atom vendor.

Hyperfine / clock-state qubit

enc_hf · layer 2 Encoding · demonstrated · since 1995

Ground-state hyperfine (or nuclear-spin) levels of atoms and ions; second-to-hour coherence.

Brief →

Key references

[104] P. Wang et al., “Single ion-qubit exceeding one hour coherence time,” Nat. Commun., vol. 1… · 2021
[374] C. R. Monroe, D. M. Meekhof, B. E. King, W. M. Itano, and D. J. Wineland, “Demonstration o… · 1995
[103] M. C. Smith, A. D. Leu, K. Miyanishi, M. F. Gely, and D. M. Lucas, “Single-qubit gates wit… · 2025
[97] A. Ransford et al., “A 98-qubit trapped-ion quantum computer with all-to-all connectivity,… · 2026
[138] H. J. Manetsch, G. Nomura, E. Bataille, K. H. Leung, X. Lv, and M. Endres, “A tweezer arra… · 2025

Design space — attributes

(a) carrier affinity
natural
(b) time · entangling
—
(c) readout
—
(d) mobility
—
(e) control
—
(f) error structure
stochastic Pauli, leakage
(g) manufacturing
—

Evaluation space — dated attributes

leakage per 1Q Clifford (Helios) → 1.1×10⁻⁵
defines: error channel · 2025-11 · source

Edges

needs: Trapped atomic ion°, Alkali atom (Rb/Cs) in optical tweezers°, Alkaline-earth(-like) atom (Yb/Sr) — erasure-native°
alternatives: Metastable ('omg') erasure encoding, Optical narrow-line qubit (ion S–D, atom clock), Ground–Rydberg analogue qubit
conflicts with:
Fluorescence imaging of atom arrays mitigated at small scale
same-species imaging light scattered and re-absorbed dephases the hyperfine data atoms
price a mid-circuit image of one atom scatters resonant light that the stored hyperfine qubits absorb; without separation or shelving the data qubits decohere during every measurement
mitigation a separate readout zone reached by transport (cx_aod), a second species, or shelving the data qubits in metastable levels (enc_omg) · 2023-05
fluorescence-detection light reaches spectator ions during mid-circuit readout
price detection light on one ion reaches its neighbours in the same chain; mid-circuit measurement of a hyperfine qubit therefore needs distance or a hidden manifold
mitigation zoned QCCD traps that move the measured ion away (cx_qccd), a second species, or metastable shelving (enc_omg) · 2021-04
° one of several that would do · the usual route, not a strict need

Used by 45 machines (44 primary · 1 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.

Extended Data Fig. 1 — Extended Data Fig. 1 Atomic-level diagram and pulse sequence.a, Level diagram showing key levels of 87Rb used in our quantum circuits.…
Two-panel figure. (a) Level diagram of rubidium-87: the qubit is the hyperfine clock pair |0⟩ = |F=1, mF=0⟩ and |1⟩ = |F=2, mF=0⟩ of 5S1/2, 6.8 GHz apart, rotated by a 795 nm Raman laser; 420 nm and 1013 nm lasers excite |1⟩ through 6P3/2 to the 53S1/2 Rydberg state |r⟩ for the entangling gate. (b) A two-qubit circuit and its laser timing: composite (BB1) Raman pulses, one CZ pulse, and a 780 nm push-out and image for readout. It is Extended Data Fig. 1 of Evered et al., Nature (2023). The Rydberg state is visited only during the gate; the qubit lives in the hyperfine pair. “Extended Data Fig. 1 — Extended Data Fig. 1 Atomic-level diagram and pulse sequence.a, Level diagram showing key levels of 87Rb used in our quantum circuits. The clock states, |0⟩…” by Evered et al., www.nature.com/articles/s41586-023-06481-y, CC BY 4.0 (creativecommons.org/licenses/by/4.0/)
Fig. 1 — Fig. 1: Experimental setup.a Energy levels of 171Yb+ and 138Ba+ ion and cutaway view of the μ-metal shielding enclosing octagon chamber. The shieldi…
A two-part figure of a trapped-ion memory experiment. Part (a) gives the energy levels of the ytterbium-171 ion — the qubit is the pair of ground hyperfine states 12.642812118 GHz apart — and of a barium-138 ion, around a cut-away drawing of the magnetic shield enclosing the octagonal vacuum chamber and trap. Part (b) is the control diagram: microwaves synthesised from a crystal oscillator reach the ions through a horn, while a 369 nm laser passes modulators, a shutter and acousto-optic modulators into a fibre; a photomultiplier detects fluorescence. From Nature Communications (2021) by Pengfei Wang, Kihwan Kim and co-authors, on a single-ion qubit with coherence estimated beyond one hour. “Fig. 1 — Fig. 1: Experimental setup.a Energy levels of 171Yb+ and 138Ba+ ion and cutaway view of the μ-metal shielding enclosing octagon chamber. The shielding has ten…” by Wang et al., www.nature.com/articles/s41467-020-20330-w, CC BY 4.0 (creativecommons.org/licenses/by/4.0/)
Fig. 1 — Figure 1: Illustration of EIT-based fast adiabatic CNOT gates with HISs. (a) shows the atomic energy levels in e.g., Cs atoms. The control qubit ato…
Schematic drawing of an energy-level scheme for a two-atom quantum gate. Panel (a) shows a control and a target caesium atom: the target qubit is stored in two hyperfine 'clock' levels of the ground state (6S1/2, F=3 and F=4), and laser fields couple it through two hyperfine intermediate levels to a highly excited Rydberg level; panels (b1) and (b2) sketch how atomic populations stay or transfer. From arXiv 2606.11655 by Fan, Zhao, Zhang, Xie and Qian, a theory proposal for fast adiabatic CNOT gates. It shows how a hyperfine qubit in a neutral atom is entangled through the Rydberg interaction. “Fig. 1 — Figure 1: Illustration of EIT-based fast adiabatic CNOT gates with HISs. (a) shows the atomic energy levels in e.g., Cs atoms. The control qubit atom is…” by Jiayin Fan, Xingdong Zhao, Manqi Zhang, Fangfang Xie, Jing Qian, arxiv.org/abs/2606.11655, CC BY 4.0 (creativecommons.org/licenses/by/4.0/)
enc_hf · layer 2 Encoding · centrality 7.2 · demonstrated · since 1995 · updated 2026-09-03

Hyperfine / clock-state qubit

Two ground-state hyperfine or nuclear-spin sublevels at a field-insensitive clock point, the default qubit for every trapped-ion and neutral-atom vendor.

Verdict. The least differentiating layer in the ion/atom stack — universal, so no moat and no lock-out; the contest is one layer up, in how the qubit is driven.

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

Two hyperfine (or nuclear-spin) ground-state sublevels at a bias field where the first-order Zeeman shift vanishes, leaving only the quadratic term: coherence in seconds to hours, with single-ion memories reaching hour scale [104]. The lineage is the field's own: NIST's first ion-trap logic gate stored a qubit in the internal states of one laser-cooled ion (Monroe, Meekhof, King, Itano, Wineland, PRL 75, 4714, 1995) [374], the default for ions and later atoms ever since.
f = Pauli + leakage — leakage into neighbouring sublevels, invisible to a Pauli decoder; reach: four architectures, QCCD and electronic-gate ions, alkali atoms, and alkaline-earth and alkaline-earth-like atoms (Sr, Yb) [graph].

Physics & limits

The clock point kills first-order field sensitivity; what remains is the quadratic Zeeman term plus field gradients across the register, so memory degrades with register size, not only time. The memory is not the limit — the drive is. Raman gates carry a spontaneous-scattering error falling only as ~1/Δ, and the scattered photon usually lands outside the qubit manifold: leakage, not Pauli error. Deleting the laser deletes that term — 2Q 99.97(1)%, 1Q 99.99916(7)% on a ten-qubit seven-zone trap Dfact, 8.4×10⁻⁵ without ground-state cooling D[102]. The control modality moves the floor, not the encoding.

Engineering state of the art

table
Date Figure Who Tag+key
2024-12-05 ⁴³Ca⁺ clock qubit, chip microwave resonator, room temperature, unshielded: 1.5(4)×10⁻⁷ per Clifford, T2 ≈ 70 s Oxford D[103]fact
2025-11 Helios fleet (98 Ba⁺): 1Q 2.5×10⁻⁵, 2Q 7.9×10⁻⁴, leakage 1.1×10⁻⁵ per Clifford Quantinuum D[97]

On atoms, Cs hyperfine T2 = 12.6 s in a 6,100-atom array D[138]. Fleet-scale term: two-qubit-gate leakage, ~10⁻⁵ per Clifford on ions against ~10⁻⁴ per atom per gate on arrays.

The PatSnap counts mix patents and papers. Not published: the isotope and transition of the hour-scale Yb⁺ memory, which its abstract calls "a single Yb ion-qubit memory"; a multi-qubit fleet-average equivalent of Oxford's 1.5(4)×10⁻⁷; and a dated supplier of isotopically enriched ¹³⁷Ba or ¹⁷¹Yb, so the enrichment chokepoint is unconfirmed.

Manufacturing, materials & supply chain

No dedicated process; the encoding rides whatever surrounds the species (Ba⁺, Yb⁺, Ca⁺, Cs, Rb, Sr). Two control families, two supply chains: Raman gates need the optical stack — Helios runs seven-plus wavelengths across 1,228 electrodes — while chip microwave traces delete it and move the burden to trap fabrication, internalised by IonQ's SkyWater purchase C[19]; eleQtron sells the same idea as MAGIC C[129]. Enriched ¹³⁷Ba and ¹⁷¹Yb are the plausible chokepoint, but no dated supplier fact was found; no specific ECCN.

Role in the stack

Architectures: the primary encoding of all three trapped-ion architectures (QCCD; linear Paul trap with individual laser addressing; electronic qubit control) and of the alkali Rydberg tweezer array, and the alternate on the alkaline-earth tweezer array. Requires nothing — the base encoding, the most reused node in the tree. Its "replaces" edge to omg is an extension: omg keeps these ground states and adds a metastable manifold so one species supplies qubit, ancilla and coolant fact. It adds nothing to the derived clock, set on the QCCD architecture by transport — a 9.66 ms round against the measured ~55 ms full-width layer (≈18 layers/s) and a 70 µs gate. Verification: Oxford's 1.5(4)×10⁻⁷ is one qubit in a dedicated apparatus, Quantinuum's 2.5×10⁻⁵ a 98-ion fleet average — three orders apart; only the fleet number is an architectural input.

Actors & economics

Who.
Organisation Role Country What exactly Evidence
Quantinuum developer US Helios, 98 Ba⁺ qubits D[97]
IonQ developer US Electronic gates, own trap fab D[102]C[19]
University of Oxford research UK ⁴³Ca⁺ single-qubit record D[103]
Atom Computing developer US Yb nuclear-spin clock qubits C[154]

Money.
2026-06-03 · Quantinuum · IPO, Nasdaq QNT, after a Sep-2025 round at $10 B pre-money · $1.68 B gross · closed Cfactfact
2026-07-31 · IonQ · SkyWater acquisition closed · ~$1.8 B Cfact

Market & supply chain. Nothing is sold as "hyperfine encoding": the money is in the drive, laser chains against microwave traps. Concentration is low in optics, rising in traps now IonQ owns a fab. Pays G3/G4/G7, the substrate under nearly every logical qubit yet demonstrated.

IP & standards. PatSnap Eureka (2026) ranks IonQ first among named assignees, 9+ records (5 JP, 2 EP, 2 IL pending) on gate pulses and motional modes; the count mixes patents with papers P[375].

Roadmaps & track record. Quantinuum: Sol 2027, Apollo 2029 (promised 2024-09-10); Helios on schedule 2025-11-05, 10×/year quantum volume held. IonQ: 256 qubits at 99.99% slipped to H1 2027, and 4,000 qubits by 2026 (promised 2020) missed ~40×. Quantinuum delivers dates, IonQ physics.

Strategic reading. Universality is the point: everyone uses it, so it is neither moat nor lock-out. The contest is the drive. If all-electronic control scales past ten qubits the laser chain becomes a liability for Quantinuum and every atom vendor; if not, IonQ bought a foundry for a lab result.

Outlook & open questions

Confirm if all-electronic control reaches a fleet average below 10⁻⁵ with published leakage, or a second group replicates 8.4×10⁻⁵; demote if it stays a ten-qubit result. Best case 2029: microwave-driven hyperfine qubits the default. Worst case: gradient-limited leakage caps ions near 10⁻⁵ and omg takes the base.

References
  1. [19] IonQ, “IonQ Completes Acquisition of SkyWater Technology,” Jul. 31, 2026. [Online]. Available: https://www.ionq.com/news/ionq-completes-acquisition-of-skywater-technology C
  2. [97] A. Ransford et al., “A 98-qubit trapped-ion quantum computer with all-to-all connectivity,” Nature, vol. 655, no. 8121, pp. 81–86, Jun. 2026, doi: 10.1038/s41586-026-10676-4. arXiv:2511.05465. D
  3. [102] A. C. Hughes et al., “Trapped-ion two-qubit gates with >99.99% fidelity without ground-state cooling,” arXiv:2510.17286, Oct. 2025. D
  4. [103] M. C. Smith, A. D. Leu, K. Miyanishi, M. F. Gely, and D. M. Lucas, “Single-qubit gates with errors at the 10⁻⁷ level,” Phys. Rev. Lett., vol. 134, no. 23, Art. no. 230601, Jun. 2025, doi: 10.1103/42w2-6ccy. arXiv:2412.04421. D
  5. [104] P. Wang et al., “Single ion-qubit exceeding one hour coherence time,” Nat. Commun., vol. 12, Art. no. 233, Jan. 2021, doi: 10.1038/s41467-020-20330-w. arXiv:2008.00251. D
  6. [129] A. Cordes, “Quantum computing scale-up eleQtron secures €57 million in one of the largest Series A funding rounds worldwide,” eleQtron, May 5, 2026. [Online]. Available: https://eleqtron.com/en/quantum-computing-scale-up-eleqtron-secures-57-million-in-one-of-the-largest-series-a-funding-rounds-worldwide/ C
  7. [138] H. J. Manetsch, G. Nomura, E. Bataille, K. H. Leung, X. Lv, and M. Endres, “A tweezer array with 6100 highly coherent atomic qubits,” Nature, vol. 647, pp. 60–67, 2025, doi: 10.1038/s41586-025-09641-4. arXiv:2403.12021. D
  8. [154] Atom Computing, “Atom Computing Raises More Than $300 Million to Accelerate Deployment of Fault-Tolerant, Neutral-Atom Quantum Computers,” PR Newswire, Jun. 16, 2026. [Online]. Available: https://www.prnewswire.com/news-releases/atom-computing-raises-more-than-300-million-to-accelerate-deployment-of-fault-tolerant-neutral-atom-quantum-computers-302800832.html C
  9. [374] C. R. Monroe, D. M. Meekhof, B. E. King, W. M. Itano, and D. J. Wineland, “Demonstration of a Fundamental Quantum Logic Gate,” Phys. Rev. Lett., vol. 75, no. 25, pp. 4714–4717, Dec. 1995, doi: 10.1103/PhysRevLett.75.4714. D
  10. [375] PatSnap, “Trapped Ion Quantum Computing: Technology Landscape 2026,” Apr. 23, 2026. [Online]. Available: https://www.patsnap.com/resources/blog/rd-blog/trapped-ion-quantum-computing-2026-patsnap-eureka/ P

G Smith, Leu, Miyanishi, Gely, Lucas (Oxford), "Single-qubit gates with errors at the 10^-7 level", arXiv:2412.04421 (2024-12-05, rev 2025-05-28): 43Ca+ hyperfine clock qubit in a mi… · 2024-12-05 · https://arxiv.org/abs/2412.04421
G Loschnauer, Mosca Toba, Hughes, King, Weber, Srinivas, Matt, Nourshargh, Allcock, Ballance, Matthiesen, Malinowski, Harty, "Scalable, high-fidelity all-electronic control of trappe… · 2024-07-10 · https://arxiv.org/abs/2407.07694
G Allcock, Campbell, Chiaverini, Chuang, Hudson, Moore, Ransford, Roman, Sage, Wineland, "omg blueprint for trapped ion quantum computing with metastable states", Applied Physics Let… · 2021 · https://cua.mit.edu/dev_site/publications/omg-blueprint-for-trapped-ion-quantum-computing-with-metastable-states
G Quantinuum raised $600 M at a $10 B pre-money valuation (NVentures, Quanta, QED, JPMorgan), 2025-09-04 · 2025-09-04 · https://www.honeywell.com/us/en/news/press-releases/2025/09/honeywell-announces-600-million-capital-raise-for-quantinuum-at-10b-pre-money-equity-valuation-to-advance-quantum-computing-at-scale
G Quantinuum IPO priced 2026-06-03: 28,000,000 shares at $60 = $1.68 B gross, Nasdaq QNT; Q2-2026 revenue $8.0 M, cash $2.1 B, FY guidance $28–32 M · 2026-06-03 · https://www.quantinuum.com/press-releases/quantinuum-announces-pricing-of-upsized-initial-public-offering
G IonQ acquired SkyWater Technology: $15.00 cash + 0.4883 IonQ shares per share (~$1.8 B at announcement 2026-01-26), closed 2026-07-31 · 2026-07-31 · https://www.ionq.com/news/ionq-completes-acquisition-of-skywater-technology