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Fermion-parity encoding (tetron) enc_parity

One logical qubit in the fermion parity of four Majorana zero modes on two wires; Z and X are parities of different mode pairs, both non-local.

Fermion-parity encoding (tetron)

enc_parity · layer 2 Encoding · theory / design only · since 2025

Qubit in joint parity of two Majorana wires; X-measurement lifetime 1000× shorter than Z in 2025 data.

Brief →

Key references

[421] T. Karzig et al., “Scalable designs for quasiparticle-poisoning-protected topological quan… · 2017
[21] M. Aghaee et al., “20 Second Parity Lifetime in an InAs–Pb Tetron Device,” arXiv:2606.0388… · 2026
[20] M. Aghaee et al., “Distinct Lifetimes for X and Z Loop Measurements in a Majorana Tetron D… · 2025

Design space — attributes

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

Evaluation space — dated attributes

Z / X parity lifetimes → 12.4 ms / 14.5 µs in the quoted tuning (~9.3 ms / ~4 µs in others; the ~10³ ratio is robust, the point values are not)
defines: error channel · 2025-07 · source

The gap is attributed to the larger quasiparticle-capture cross-section of the two-wire X loop — flux noise is not the stated cause. DARPA US2QC: final Validation & Co-Design stage since 2025-02-06, not QBI Stage B.

Actors & goals — annotations

Edges

needs: Majorana parity (InAs–Pb tetron)
needed by: Measurement-based Majorana gate
° one of several that would do · the usual route, not a strict need

Used by 2 machines (2 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: Schematic of the sparse encoding for a single qubit, with the logical qubit labelled along with the parity conserving ancilla. Hybridizati…
A simple drawn schematic, not a picture of a device: four Majorana modes γ1–γ4, two boxed as the qubit and two as a parity-conserving ancilla, with arcs marking Z and X couplings. It is Figure 1 of the arXiv paper "Majorana braiding simulations with projective measurements" by Philipp Frey, Themba Hodge, Eric Mascot and Stephan Rachel. It illustrates fermion-parity (tetron-style) encoding: the qubit is stored in the joint parity of Majorana pairs, and letting pairs hybridize rotates the qubit state continuously. “Fig. 1 — Figure 1: Schematic of the sparse encoding for a single qubit, with the logical qubit labelled along with the parity conserving ancilla. Hybridization between…” by Philipp Frey, Themba Hodge, Eric Mascot, Stephan Rachel, arxiv.org/abs/2508.10106, CC BY 4.0 (creativecommons.org/licenses/by/4.0/)
Fig. 1 — Figure 1: (a) Sketch of the poor man’s tetron: two semiconducting nanowires (blue) are connected by a shared SC floating island (silver); a set of e…
A two-panel drawing, not a photograph: a 3D render of two semiconductor nanowires joined by a shared superconducting floating island, with gate-defined quantum dots, gold gates and four leads, and a schematic of the model's Hamiltonian terms. It is Figure 1 of the arXiv paper "The poor man's Majorana tetron" by Maximilian Nitsch and co-authors. It illustrates a minimal Majorana tetron qubit built from coupled quantum dots; per the caption, the four leads are used to explore the emerging Kondo physics. “Fig. 1 — Figure 1: (a) Sketch of the poor man’s tetron: two semiconducting nanowires (blue) are connected by a shared SC floating island (silver); a set of…” by Maximilian Nitsch et al., arxiv.org/abs/2411.11981, CC BY 4.0 (creativecommons.org/licenses/by/4.0/)
Fig. 1 — Figure 1: Braiding geometries and protocols. (a) Trijunction network and (b) quantum-dot-assisted architecture, showing the device layout to exchang…
Shaded schematic drawings, not device images, of two ways to exchange (braid) Majorana zero modes: a T-shaped nanowire junction with modes γ1-γ4 at the wire ends, and two wire segments linked by a quantum dot, each with step-by-step frames of the exchange. From "Noisy Braiding of Majorana Modes: A Comparison of Nanowire Trijunction and Quantum-Dot-Assisted Architectures" by Dibyajyoti Sahu and Suhas Gangadharaiah. Braiding is the intended gate operation of topological qubits; notice the modes moving along wire arms in one design and through the dot in the other. “Fig. 1 — Figure 1: Braiding geometries and protocols. (a) Trijunction network and (b) quantum-dot-assisted architecture, showing the device layout to exchange the…” by Dibyajyoti Sahu, Suhas Gangadharaiah, arxiv.org/abs/2608.09416, CC BY 4.0 (creativecommons.org/licenses/by/4.0/)
enc_parity · layer 2 Encoding · centrality 4.2 · theory / design only · since 2025 · updated 2026-09-04

Fermion-parity encoding (tetron)

One logical qubit in the fermion parity of four Majorana zero modes on two wires; Z and X are parities of different mode pairs, both non-local.

Verdict. Not a working encoding as of 4 Sep 2026 — its X channel lives ~1000× shorter than its Z channel; falsified as fault-tolerance-relevant unless that ratio falls below 10× by 2028.

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

Four Majorana zero modes (MZMs) on two wires joined by a superconducting backbone hold one qubit: Z is the parity of one wire's mode pair, X of a pair spanning both, so neither logical operator is local. Karzig et al. defined the tetron and hexon layouts in 2017, with Cliffords by measurement rather than braiding S[421]. Only Z-type parity has been read with a stated fidelity; the X measurement the encoding requires has not D[21].
a fabricated (1.0) · b not a gate · c no readout · d no transport
e no control · f asymmetric, poisoning-dominated · g inherits the wire fab

Physics & limits

Protection is a length and a gap: parity splitting falls exponentially with length over coherence length, poisoning as the gap rises against temperature and quasiparticle density S[421]. Neither is published. Published instead: 12.4 ms on the Z loop against 14.5 µs on the X loop in one device D[20]. Both are fermion parities, so the ~1000× factor is geometric: the X loop encloses both wires and captures quasiparticles over a larger cross-section D[20]. A code needs comparable rates on both bases, and this is not usable bias: the short basis is the one a measurement-based gate projects most. Moving the floor means a larger gap (lead replaced aluminium D[21]), quasiparticle trapping and a smaller X loop.

Engineering state of the art

table
Year Figure Who Tag+key
2017 Tetron and hexon layouts defined; measurement-only Cliffords Microsoft S[421]
2025-07 Z loop 12.4 ms vs X loop 14.5 µs, one tetron Microsoft Quantum D[20]
2026-06 One wire of one tetron in an array; no joint parity Microsoft Quantum D[21]

No logical state prepared, no X measurement, no coherence time or logical error rate for a tetron D[21].

The arXiv text of [20] also gives X ~4 µs and Z ~9.3 ms for other tunings, against the 14.5 µs / 12.4 ms quoted above. No non-Microsoft tetron exists. Not published: a Majorana splitting, a wire length over coherence length or a quasiparticle density for any tetron, so the protection claim cannot be checked numerically; and whether the X/Z asymmetry is geometric or intrinsic.

Manufacturing, materials & supply chain

No process of its own; the encoding fixes a geometry. Two wires, a backbone and the dots closing each loop cost more area and steps than a bare wire, and the X loop's coupling elements are exactly what a Z-only measurement avoids. Bring-up is per device: the 2026 rf technique resolves wire-end-state splitting to µeV so array devices can be tuned at all D[21]. Below it is in-house InAs–Pb epitaxy, unreplicated outside Microsoft; no export-control category specific to it.

Role in the stack

Architecture: topological — tetron (Majorana), where it is the primary encoding. It requires two wires per qubit and supplies the logical degree of freedom a measurement-based gate would act on; nothing else consumes it, and it sets no clock. Verification is one-sided: telegraph statistics on parity loops, no logical error per cycle, no Λ, no independent tetron. The dispute runs deeper: Legg's Matters Arising (2026-06-24) argues the regions read out in 2025 were disordered and gapless, making the encoded object trivial rather than protected; Microsoft's same-day reply concedes nothing D[22]. QuTech's parity qubit in coupled Kitaev chains is an alternative encoding with limited protection, not a tetron replication D[217].

Actors & economics

Who.
| Organisation | Role | Country | What they do | Evidence |
|---|---|---|---|---|
| Microsoft Quantum | developer | US | Defined the tetron and holds the only Z/X data | D[20] |
| DARPA | investor | US | US2QC final Validation & Co-Design stage since 2025-02-06 | fact |
| QuTech | research | NL | Competing parity encoding in coupled Kitaev chains | D[217] |
| Nokia Bell Labs | research | US | Fractional-quantum-Hall anyon route, a different encoding | Dfact |

Money. 2025-02-06 · Microsoft · US2QC final Validation & Co-Design stage · undisclosed · DARPA · announced fact. 2026-01-23 · Microsoft · Quantum Pioneers Program, QEC an award topic · ≤ USD 200,000 per proposal · announced Pfact.

Market & supply chain. Nothing is sold; it consumes wires and readout and pays back only in G4, after an X measurement exists.

IP & standards. The tetron layout is Microsoft's published lineage S[421]; no dated patent count specific to it as of 4 Sep 2026.

Roadmaps & track record. (tetron as the fault-tolerance unit, promised 2017, restated for 2029 in 2026; status 4 Sep 2026: no X measurement, no logical qubit) C[215]. Nine years from design to a one-wire measurement, with no interim milestone for the X/Z ratio.

Strategic reading. Every topological claim above sits on this ratio. If it closes, Microsoft's fabrication lead becomes a code; if not, the tetron gives way to a longer Kitaev chain and the wire stack loses its justification. Risk is single-vendor and single-design.

Outlook & open questions

Falsifiable in 12–24 months: any X-basis parity measurement with a stated assignment error; an X/Z ratio below 100×; a joint measurement across two tetrons. Confirm on the first two; demote to theory if none appears by end-2027. Best case, loop redesign and a larger gap bring X into milliseconds; worst case, X-loop poisoning is intrinsic and the design is abandoned. Open: is the asymmetry geometric or intrinsic; does anyone build a tetron outside Microsoft.

References
  1. [20] M. Aghaee et al., “Distinct Lifetimes for X and Z Loop Measurements in a Majorana Tetron Device,” arXiv:2507.08795, Jul. 2025. D
  2. [21] M. Aghaee et al., “20 Second Parity Lifetime in an InAs–Pb Tetron Device,” arXiv:2606.03884, Jun. 2026. D
  3. [22] H. F. Legg, “On the robustness of topological gap detection via transport,” Nature, vol. 654, no. 8120, pp. E22–E26, Jun. 2026, doi: 10.1038/s41586-026-10567-8. arXiv:2503.08944. D
  4. [215] C. Nayak, “Majorana 2 – Microsoft's Scalable Quantum Processor With Reliable, Long-Lasting Qubits,” Microsoft Quantum. [Online]. Available: https://quantum.microsoft.com/en-us/insights/blogs/majorana-2-scalable-quantum-processor C
  5. [217] F. Zatelli et al., “Majorana parity qubit in coupled minimal Kitaev chains,” arXiv:2607.09511, Jul. 2026. D
  6. [421] T. Karzig et al., “Scalable designs for quasiparticle-poisoning-protected topological quantum computation with Majorana zero modes,” Phys. Rev. B, vol. 95, no. 23, Art. no. 235305, Jun. 2017, doi: 10.1103/PhysRevB.95.235305. arXiv:1610.05289. S