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Cat-code encoding (biased noise) enc_cat

A two-photon-dissipation-stabilised coherent-state qubit whose bit-flips fall exponentially with photon number while phase-flips rise linearly with it.

Cat-code encoding (biased noise)

enc_cat · layer 2 Encoding · demonstrated · since 2020

Two-photon-dissipation-stabilised coherent states; bit-flips exponentially suppressed, phase-flips grow ∝ n̄.

Brief →

Key references

[80] H. Putterman et al., “Hardware-efficient quantum error correction via concatenated bosonic… · 2025
[77] N. Coppola, “Alice & Bob Shares Preliminary Results Vastly Surpassing Previous Bit-Flip Ti… · 2025
[78] N. Coppola, “Alice & Bob Improves Error Suppression in Quantum Computers by 'Squeezing' Ca… · 2025
[65] DARPA, “Stage B selection,” Nov. 6, 2025. [Online]. Available: https://www.darpa.mil/resea… · 2025

Design space — attributes

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

Evaluation space — dated attributes

bit-flip time → 44 min mean (12-cat chip, preliminary); 22 s squeezed cat
defines: error channel · 2025-09 · source
phase-flip per CX (Ocelot) → 9.6(4)×10⁻² at n̄=2 (bit-flip 3.5(4)×10⁻³); bias > 25 under the gate, > 30 idle
defines: error channel · 2025-02 · source

Alice & Bob (DARPA QBI Stage A only), AWS. The '27–33' figures quoted elsewhere are phase-flip *times* in µs, not bias values.

Actors & goals — annotations

Edges

needs: Bosonic cavity mode
needed by: Bias-preserving cat–cat CNOT, Bosonic concatenation (repetition-cat, LDPC-cat, GKP+qLDPC)°
alternatives: Bare physical qubit (no encoding), GKP grid encoding
conflicts with:
Rotated surface code (+ yoked variants) bypassed by choosing another technology in place of one of the two
unbiased code wastes the bias — needs repetition/XZZX/elevator codes
price a CSS surface code corrects X and Z symmetrically, so a bias > 25 (Ocelot, 2025) buys nothing; the ~10× qubit saving of cat architectures exists only with bias-tailored codes
mitigation repetition (Ocelot), XZZX, elevator or LDPC-cat codes instead of the plain surface code · 2025-02
° one of several that would do · the usual route, not a strict need

Used by 5 machines (5 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: Kerr-cat qubit encoding and 2D chip architecture. (a) The Bloch sphere for the Kerr-cat qubit is spanned by the cat states along the x-axi…
Seven-panel paper figure: theory drawings of the Kerr-cat qubit (Bloch sphere, double-well potential, photon-number distribution), a circuit diagram, and a real false-coloured optical micrograph of the square chip (1 mm scale bar) with SNAIL-based qubit pads, filters and meandering readout resonators. From the arXiv paper "High-Coherence Kerr-cat qubit in 2D architecture" by Ahmed Hajr and co-authors. It illustrates a superconducting cat-code qubit built from two opposite-phase coherent states, which makes bit flips rare; notice the Purcell filters that shield the qubit from its readout line. “Fig. 1 — Figure 1: Kerr-cat qubit encoding and 2D chip architecture. (a) The Bloch sphere for the Kerr-cat qubit is spanned by the cat states along the x-axis and the…” by Ahmed Hajr et al., arxiv.org/abs/2404.16697, CC BY 4.0 (creativecommons.org/licenses/by/4.0/)
Fig. 1 — Figure 1: (a) Schematic of the setup: Two cavities are coupled through a Josephson junction. A weak resonant drive εb and a strong off-resonant p
A two-panel drawing, not a device. (a) A low-Q readout cavity (blue) coupled through a Josephson junction to a high-Q storage cavity (red), each with a port (wavy arrows); (b) the storage cavity's states drawn as a sphere whose poles are the cat states |C+⟩ and |C−⟩ (Wigner-function icons), purple arrows pushing every state toward it. It is Figure 1 of arXiv 2609.15477, 'Engineering dissipation and control pulses for high-fidelity fault-tolerance quantum computing', by Shao-Wei Xu and co-authors. It illustrates cat-code encoding in a superconducting bosonic cavity mode: a weak resonant drive and a strong off-resonant pump create engineered dissipation that steers states into the protected cat subspace. “Fig. 1 — Figure 1: (a) Schematic of the setup: Two cavities are coupled through a Josephson junction. A weak resonant drive εb and a strong off-resonant…” by Shao-Wei Xu, Zhe-Yuan Zhang, Yi-Tong Shi, Ye-Hong Chen, Yan Xia, arxiv.org/abs/2609.15477, CC BY 4.0 (creativecommons.org/licenses/by/4.0/)
Fig. 1 — Figure 1: Generalized photon subtraction in picosecond wave packets for high-rate non-Gaussian-resource generation. (a) Generalized photon subtracti…
An optical drawing and two plots. (a) Generalized photon subtraction: two squeezed light beams meet on a beam splitter, and a photon-number-resolving detector heralds a squeezed 'Schrödinger cat' state (a superposition of two opposite coherent states), which is then adaptively squeezed; an inset contrasts conventional nanosecond-spaced pulses with picosecond ones; (b) quadrature versus phase for a plus cat (α=1.5), showing the 'alive' and 'dead' parts interfering; (c) its Wigner function with negative fringes. From arXiv 2606.24002, 'Picosecond Schrödinger cat states for ultrafast optical quantum processing', by Endo, Takase, Furusawa and co-authors. Cat states feed cat codes and GKP (Gottesman–Kitaev–Preskill) qubits in optical quantum computing; shorter pulses allow faster clock rates. “Fig. 1 — Figure 1: Generalized photon subtraction in picosecond wave packets for high-rate non-Gaussian-resource generation. (a) Generalized photon subtraction (GPS) is…” by Mamoru Endo et al., arxiv.org/abs/2606.24002, CC BY 4.0 (creativecommons.org/licenses/by/4.0/)
enc_cat · layer 2 Encoding · centrality 7.4 · demonstrated · since 2020 · updated 2026-09-30

Cat-code encoding (biased noise)

A two-photon-dissipation-stabilised coherent-state qubit whose bit-flips fall exponentially with photon number while phase-flips rise linearly with it.

Verdict. The bias is real but small where measured — bias > 25 under a CX at n̄ = 2; the resource estimates imply a cavity lifetime near 50 ms, twice the best ever built.

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 qubit spanned by two coherent states of a cavity mode, held there by engineered two-photon exchange with a lossy buffer. Bit-flips must cross phase space between the lobes, exponentially suppressed in n̄; one photon loss flips the phase, linear in n̄. Demonstrated from about 2020 (Lescanne, Leghtas and colleagues), commercialised by Alice & Bob and AWS. It has no gate time or readout of its own; its only product is the asymmetry.

Physics & limits

Γ_Z ≈ n̄/T1: the encoding turns cavity lifetime directly into logical quality, and photon number buys bit-flip suppression at a linear price. Ocelot closes the loop: at n̄ = 2 the storage lifetime is 57–68 µs D[80]. Run that arithmetic at the operating point the estimates assume, n̄ ≈ 19 and 10⁻³ phase-flip per cycle, and the required cavity T1 is n̄·t/p ≈ 53 ms S[80], [95]. The best published cavity memory is 25.6 ms, built by decoupling the mode from its ancilla — the opposite of what a stabilised cat does D[319]. That is the floor: the qubit-count argument is a claim about cavity lifetime under strong drive. What moves it: lower single-photon loss at high pump power, or squeezed cats D[78].

Engineering state of the art

table
Date Figure Who Tag
2025-02 Per CX at n̄ = 2: phase-flip 9.6(4)×10⁻², bit-flip 3.5(4)×10⁻³ → bias > 25, idle > 30; repetition code 1.75(2)% (d=3, n̄=1) → 1.65(3)% (d=5, n̄=1.5) per 2.8 µs cycle AWS/Caltech D[80]
2025-09 12-cat chip: mean bit-flip 44 min, peak 252 min, preliminary Alice & Bob C[77]
2025-02 Squeezed-cat variant: 22 s bit-flip Alice & Bob D[78]

Phase-flip dominates: ~10⁻¹ per cycle where a code has run, against the ~10⁻³ assumed; bit-flip suppression stopped being the problem two years ago.

The 9.6×10⁻² is the phase-flip error of the CX gate at n̄ = 2, not a per-QEC-cycle figure; the noise bias is > 25 under the CX and > 30 idle, and the "27–33" in circulation are phase-flip times in µs, not bias values D[80]. The 44-minute mean bit-flip time of the 12-cat chip (September 2025) is preliminary and vendor-published, with no peer-reviewed follow-up, and the vendor's roadmap page gives a 252-minute peak for the same period. The 53 ms cavity-lifetime requirement is derived from Γ_Z ≈ n̄/T1 under the estimates' own assumptions; neither source states it. Nord Quantique's QBI Stage B award [65] funds its GKP route, which does not use this encoding.

Manufacturing, materials & supply chain

It has no fabrication step of its own, adding a continuous parametric pump and buffer mode to the host cavity. That pump is the I/O cost: a drive line, a pump line and a readout chain per cat — through a shared ancilla transmon on Ocelot, through the buffer at Alice & Bob Cfact. Ocelot spends five buffers and four ancilla transmons on five cats D[80]. At 10³ cats the wall is pump-line count and pump heating in one dilution unit; 10⁴–10⁶ needs multiplexed cryogenic drive, undemonstrated here. Supply chain and export exposure are the host cavity's.

Role in the stack

Architecture: bosonic cavity qubits — cat and GKP, where it is the primary encoding. Requires a bosonic cavity mode; provides the biased inner qubit for repetition-cat and LDPC-cat concatenation and for a cat–cat CNOT. It replaces the bare two-level encoding, competes with GKP and conflicts with the unbiased surface code. Derived round 1.44 µs, gate-set, against the measured 2.8 µs syndrome cycle D[80]. Verification: the distance-3 and distance-5 points were taken at n̄ = 1 and n̄ = 1.5, so "flat with distance" mixes distance with operating point D[80]. The 44-minute mean bit-flip is preliminary; the same vendor's roadmap quotes a 252-minute peak from that run C[77]C[412].

Actors & economics

Who.
Organisation Role Country What exactly they do Evidence
Alice & Bob developer FR Bit-flip records, 18-cat Helium, a cat-only roadmap C[77]
AWS developer US Ocelot, the only published cat code with a budget D[80]
DARPA investor US Stage B selected Nord Quantique, not Alice & Bob fact

Money.
2025-01-28 · Alice & Bob · Series B · €100 M · — · closed fact
2026-05-22 · Alice & Bob · Series B extension · undisclosed · NVentures lead · closed C[88]

Market & supply chain. Nothing is sold at this layer; the encoding is a design choice on the cavity supply chain, bought as a promise about G3 and G4. Alice & Bob's business rests on it.

IP & standards. No dated patent family specific to cat-code encoding was found; filings attach to gates, pumps and readout.

Roadmaps & track record. The published ladder runs Helium (18 cats, 1 logical, 10⁻², delivered 2026-06) → Lithium (48/4, 10⁻³) → Beryllium (250/5, 10⁻⁴) → Graphene (2,000/100, 10⁻⁶, 2030) R[412]. Chips arrive on time, but no logical error rate has been published for any, so every defining number is a promise. AWS has published no cat roadmap past Ocelot.

Strategic reading. If phase-flip per cycle falls two orders, cat encoding wins the physical-qubit count; if not, the branch is a memory technology and the budget goes to qLDPC or dual-rail erasure.

Outlook & open questions

Confirm by 2027 if phase-flip per cycle falls below 10⁻² with bias above 100 at fixed n̄; demote the efficiency claims if it stays near 10⁻¹. Best case 2029: a cat at n̄ ≥ 5 with millisecond lifetime under active stabilisation. Worst case: bias saturates and the 758-cat and 126,133-cat estimates stay unreachable S[95], [96]. Open: does squeezing survive multi-qubit operation; can pump power rise without loading T1? Watch Lithium and any Ocelot successor.

References
  1. [65] DARPA, “Stage B selection,” Nov. 6, 2025. [Online]. Available: https://www.darpa.mil/research/programs/quantum-benchmarking-initiative/stage-b-selection G
  2. [77] N. Coppola, “Alice & Bob Shares Preliminary Results Vastly Surpassing Previous Bit-Flip Time Record,” Alice & Bob, Sep. 25, 2025. [Online]. Available: https://alice-bob.com/newsroom/alice-bob-surpasses-bit-flip-stability-record C
  3. [78] N. Coppola, “Alice & Bob Improves Error Suppression in Quantum Computers by 'Squeezing' Cat Qubits,” Alice & Bob, Mar. 11, 2025. [Online]. Available: https://alice-bob.com/newsroom/squeezed-cat-qubit/ D
  4. [80] H. Putterman et al., “Hardware-efficient quantum error correction via concatenated bosonic qubits,” Nature, vol. 638, no. 8052, pp. 927–934, Feb. 2025, doi: 10.1038/s41586-025-08642-7. D
  5. [88] N. Coppola, “Alice & Bob announces Series B Extension,” Alice & Bob, May 22, 2026. [Online]. Available: https://alice-bob.com/newsroom/alice-bob-announces-series-b-extension/ C
  6. [95] É. Gouzien, D. Ruiz, F.-M. Le Régent, J. Guillaud, and N. Sangouard, “Performance Analysis of a Repetition Cat Code Architecture: Computing 256-bit Elliptic Curve Logarithm in 9 Hours with 126133 Cat Qubits,” Phys. Rev. Lett., vol. 131, Art. no. 040602, Jul. 2023, doi: 10.1103/PhysRevLett.131.040602. arXiv:2302.06639. S
  7. [96] D. Ruiz, J. Guillaud, A. Leverrier, M. Mirrahimi, and C. Vuillot, “LDPC-cat codes for low-overhead quantum computing in 2D,” Nat. Commun., vol. 16, Art. no. 1040, 2025, doi: 10.1038/s41467-025-56298-8. arXiv:2401.09541. S
  8. [319] O. Milul et al., “Superconducting Cavity Qubit with Tens of Milliseconds Single-Photon Coherence Time,” PRX Quantum, vol. 4, no. 3, Art. no. 030336, Sep. 2023, doi: 10.1103/PRXQuantum.4.030336. D
  9. [412] Alice & Bob, “Roadmap,” Jun. 23, 2026. [Online]. Available: https://alice-bob.com/roadmap/ C