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Bare physical qubit (no encoding) enc_bare

The {|0⟩,|1⟩} subspace of a weakly anharmonic Josephson oscillator used directly as the qubit, with no bosonic, erasure or bias structure on top.

Bare physical qubit (no encoding)

enc_bare · layer 2 Encoding · demonstrated · since 2007

Computational subspace of an anharmonic oscillator; leakage to |2⟩ is the price.

Brief →

Key references

[1] Google Quantum AI and Collaborators, “Quantum error correction below the surface code thre… · 2024
[3] T. He et al., “Experimental Quantum Error Correction below the Surface Code Threshold via … · 2025
[2] V. Sivak et al., “Reinforcement learning control of quantum error correction,” Nature, vol… · 2026
[38] F. Marxer et al., “Above 99.9% Fidelity Single-Qubit Gates, Two-Qubit Gates, and Readout i… · 2026
[34] IBM Quantum, “What's new at IBM Quantum - Q2 2026.” [Online]. Available: https://www.ibm.c…

Design space — attributes

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

Evaluation space — dated attributes

leakage suppression → 72× (all-microwave reset), residual 6.4×10⁻⁴ after 40 cycles
defines: error channel · 2025-12 · source

USTC leakage suppression = PRL 135, 260601 (2025-12-22), Λ = 1.40(6) at d=7; the paper does not name the processor 'Zuchongzhi 3.2'.

Actors & goals — annotations

Edges

needs: Transmon°, Fluxonium°
alternatives: Dual-rail (erasure) encoding, Cat-code encoding (biased noise)
° one of several that would do · the usual route, not a strict need

Used by 78 machines (78 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: (a) Simplified energy diagram of a transmon (red). The black dashed curve is the parabolic potential of a harmonic oscillator. (b) Schemat…
A four-panel figure, mostly drawings and data: a transmon energy diagram, current-phase curves for three junction types, a circuit schematic with a false-colour electron-micrograph inset of a nanowire junction (200 nm scale bar), and spectroscopy. It comes from the arXiv paper "Tunable anharmonicity in Sn-InAs nanowire transmons beyond the short junction limit" by Amrita Purkayastha and co-authors. It illustrates a transmon whose junction is a gate-tuned semiconductor nanowire; notice the anharmonicity — the unequal level spacing that lets the two lowest levels act as a qubit. “Fig. 1 — Figure 1: (a) Simplified energy diagram of a transmon (red). The black dashed curve is the parabolic potential of a harmonic oscillator. (b) Schematic…” by Amrita Purkayastha et al., arxiv.org/abs/2603.26895, CC BY 4.0 (creativecommons.org/licenses/by/4.0/)
Fig. 1 — Fig. 1: Removing leakage with reset.a Schematic of the multi-level reset protocol. The qubit starts with a population in its first three excited sta…
Drawn two-panel figure explaining a fast reset for superconducting qubits. From Nature Communications (2021), 'Removing leakage-induced correlated errors in superconducting quantum error correction', by M. McEwen, D. Kafri, Z. Chen and colleagues. Panel (a) shows energy ladders of a transmon and its readout resonator: excitations, including leaked states |2⟩ and |3⟩, are swapped into the resonator, which then decays, and the qubit returns empty — about 250 ns in all per the caption. Panel (b) places this reset R after each measurement in a bit-flip code round, where red stars mark leakage that otherwise spreads. It is a diagram, not data. “Fig. 1 — Fig. 1: Removing leakage with reset.a Schematic of the multi-level reset protocol. The qubit starts with a population in its first three excited states (closed…” by McEwen et al., www.nature.com/articles/s41467-021-21982-y, CC BY 4.0 (creativecommons.org/licenses/by/4.0/)
File:VdW qubit.png
A drawn schematic, not a built device: two atomic layers drawn as honeycomb lattices form a stack with a gate electrode V_G, two end contacts labelled A and B, and a green Bloch sphere showing a qubit state. It was posted on Wikimedia Commons by Brunolucatto on 2019-04-27 as a possible physical implementation of a van der Waals qubit. Per its caption, the gate field changes the state of a conduction-band electron in the layers; notice the equation writing that state as a superposition of A and B. “VdW qubit” by Brunolucatto, commons.wikimedia.org/wiki/File:VdW_qubit.png, CC BY SA 4.0 (creativecommons.org/licenses/by-sa/4.0/)
enc_bare · layer 2 Encoding · centrality 4.2 · demonstrated · since 2007 · updated 2026-09-04

Bare physical qubit (no encoding)

The {|0⟩,|1⟩} subspace of a weakly anharmonic Josephson oscillator used directly as the qubit, with no bosonic, erasure or bias structure on top.

Verdict. The default of every mainstream superconducting vendor as of 2026-09-04; its structural cost is leakage plus an unbiased error model, which caps measured Λ at 1.4–2.1 where erasure encodings simulate an order of magnitude higher.

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

Using the lowest two levels of a Josephson circuit directly as a qubit is as old as the Cooper-pair box (Nakamura, 1999); the transmon (Koch et al., 2007) made it the default by buying charge insensitivity with lower anharmonicity — which is what creates the leakage problem.
Attributes: it adds no characteristic time, readout, mobility, control or fabrication of its own — each is the carrier's.
Error structure as the code sees it: unbiased Pauli plus leakage out of the subspace.

Physics & limits

The scale that matters is α ≈ −EC ≈ 2π × 200–300 MHz: it sets the minimum gate time and the leakage per gate, which DRAG (derivative removal by adiabatic gate) pulse shaping suppresses but cannot remove. Raising α costs charge dispersion, which grows as exp(−√(8E_J/E_C)); that trade is the floor here. Leakage persists where a Pauli fault does not: the second excited state survives tens of QEC cycles at Willow's 1.1 µs D[1], feeding the decoder correlated wrong syndromes. Hence dedicated removal: USTC's all-microwave scheme suppresses leakage 72×, to a residual 6.4(5)×10⁻⁴ after 40 cycles D[3]. What moves the floor is leakage-aware decoding and faster multi-level reset.

Engineering state of the art

table
Date Figure Who Tag
2024-12-09 d=7 surface code, Λ = 2.14 ± 0.02 Google (Willow) D[1]
2025-12-22 Leakage suppressed 72×, Λ = 1.40(6) at d=7 USTC D[3]
2026-07-08 d=7 logical error 7.72×10⁻⁴ per cycle Google D[2]

Best in class is one characterised IQM pair, CZ 99.93% over 40 h D[38]; typical at scale is IBM's fleet EPLG 3.7×10⁻³, best 1.9×10⁻³ D[34], and Rigetti's 108-qubit median 99.1% C[36].

The 72× leakage suppression and the 6.4(5)×10⁻⁴ residual come from one USTC device, unreplicated as of 2026-09-04; the paper does not name the processor, and the "Zuchongzhi 3.2" label comes from outside it. Not published: a leakage figure for IBM's fleet, whose EPLG aggregates all error mechanisms.

Manufacturing, materials & supply chain

Nothing of its own: it inherits the carrier's 300 mm Nb/Al lithography, yield spread and one drive plus one readout line per qubit. That is the whole commercial argument — dual-rail erasure adds a rail and a check per qubit (384 ns, 2.54×10⁻² erasure D[85]), cat codes a pump and buffer mode. The I/O wall is the carrier's: coax per qubit, ~10³ qubits per fridge. What this encoding adds at 10⁴–10⁶ is leakage removal inside every 1.1 µs cycle and the decoder bandwidth to use it. Export exposure is the carrier's (US EAR ECCN 3A901).

Role in the stack

The default Layer-2 encoding on the transmon lattice with tunable couplers (IBM, Google, Rigetti, IQM, OQC, USTC/Zhejiang, Fujitsu). Dual-rail erasure or cat encoding replaces it when a vendor trades control complexity for a friendlier error structure: Alice & Bob, AWS and D-Wave/Quantum Circuits have, IBM and Google have not. The price is quantifiable: measured dual-rail gate errors simulate to Λ ≈ 27 against 14 for 0.1% depolarising noise S[84], where this encoding measures 2.14 and 1.40(6) D[1], [3]. It adds nothing to the derived clock, which stays the carrier's 0.65 µs round inside its measured 1.1 µs cycle. Verification: the 72× is one unreplicated USTC device, and leakage is self-reported with no cross-vendor protocol.

Actors & economics

Who.
Organisation Role Country What exactly they do Evidence
IBM developer US Whole fleet and the Starling roadmap on bare transmons D[34]
Google developer US Willow QEC and the d=7 logical-error record D[1]
USTC research CN Below-threshold d=7 via leakage suppression D[3]

Money.
2026-06-02 · IBM · investment commitment · > $10 B over five years · announced G[57]fact
2026-07-02 · IQM · Nasdaq and Helsinki listing · pro-forma cash €337 M · closed C[58]fact

Market & supply chain. No supply chain of its own; concentration sits one layer down, in Nb/Al lithography and dilution refrigerators. Being free, it is what every G1–G4 budget on this architecture buys.

IP & standards. No dated patent family found for bare-subspace leakage mitigation as of 2026-09-04; PatSnap's 2026-06-30 counts are not encoding-specific Pfact.

Roadmaps & track record. IBM (2025-06-10 · Starling, 200 logical / 10⁸ gates in 2029 · Nighthawk on plan, Kookaburra slipped a year fact). Google (2025 · long-lived logical qubit at 10⁻⁶ · no successor to Willow). Neither publishes a leakage target.

Strategic reading. Its edge is that it is free, so the fork is capital allocation: money spent switching to erasure is not spent scaling the bare fleet. If Λ stays near 2, erasure encodings win on physical qubits per logical; otherwise incumbents keep the field.

Outlook & open questions

Confirm by end-2027: ≥ 50× leakage suppression in a below-threshold code outside USTC, or leakage published as a line item in a vendor's logical error budget; otherwise demote it to a single-device claim. Best case 2029: leakage falls under the correlated-event floor (≈10⁻¹⁰, hourly bursts on Willow D[1]); worst case, Λ stays near 2 and physical-per-logical above 10³. Does leakage or 2Q error dominate at 10⁴ qubits? Can removal keep up at 10⁶? Does erasure conversion ever cross over commercially?

References
  1. [1] Google Quantum AI and Collaborators, “Quantum error correction below the surface code threshold,” Nature, vol. 638, no. 8052, pp. 920–926, Dec. 2024, doi: 10.1038/s41586-024-08449-y. D
  2. [2] V. Sivak et al., “Reinforcement learning control of quantum error correction,” Nature, vol. 655, no. 8124, pp. 879–884, Jul. 2026, doi: 10.1038/s41586-026-10759-2. D
  3. [3] T. He et al., “Experimental Quantum Error Correction below the Surface Code Threshold via All-Microwave Leakage Suppression,” Phys. Rev. Lett., vol. 135, no. 26, Art. no. 260601, Dec. 2025, doi: 10.1103/rqkg-dw31. D
  4. [34] IBM Quantum, “What's new at IBM Quantum - Q2 2026.” [Online]. Available: https://www.ibm.com/quantum/blog/whats-new-q2-2026 D
  5. [36] Rigetti Computing, Inc., “Rigetti Announces General Availability of 108-Qubit System,” Apr. 7, 2026. [Online]. Available: https://investors.rigetti.com/news-releases/news-release-details/rigetti-announces-general-availability-108-qubit-system C
  6. [38] F. Marxer et al., “Above 99.9% Fidelity Single-Qubit Gates, Two-Qubit Gates, and Readout in a Single Superconducting Quantum Device,” PRX Quantum, vol. 7, Art. no. 020333, 2026, doi: 10.1103/n86s-2b88. arXiv:2508.16437. D
  7. [57] IBM Quantum, “Why IBM is investing $10 billion into quantum computing,” Jun. 2, 2026. [Online]. Available: https://www.ibm.com/quantum/blog/10-billion-investment-faq G
  8. [58] IQM Quantum Computers, “IQM Quantum Computers Becomes First European Quantum Computing Company Listed on a Major U.S. Exchange,” Jul. 2, 2026. [Online]. Available: https://iqm.tech/press-releases/iqm-quantum-computers-becomes-first-european-quantum-computing-company-listed-on-a-major-u-s-exchange/ C
  9. [84] N. Mehta et al., “An entangling gate for dual-rail erasure qubits,” Nature, vol. 656, no. 8126, pp. 47–53, Aug. 2026, doi: 10.1038/s41586-026-10822-y. arXiv:2503.10935. S
  10. [85] J. S.-C. Hung et al., “Fast, High-Fidelity Erasure Detection of Dual-Rail Qubits with Symmetrically Coupled Readout,” arXiv:2604.16292, Apr. 2026. D