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rf quantum-capacitance parity readout ro_qcap

Dispersive gate sensing of a Majorana island's quantum capacitance by rf reflectometry, reading fermion parity without charge transfer; non-destructive and mid-circuit.

rf quantum-capacitance parity readout

ro_qcap · layer 6 Readout · emerging · since 2025

Interferometric parity readout of a Majorana wire; 1% assignment error, SNR 1 in 3.6 µs.

Brief →

Key references

[13] Microsoft Azure Quantum, “Interferometric single-shot parity measurement in InAs–Al hybrid… · 2025
[216] N. van Loo et al., “Single-shot parity readout of a minimal Kitaev chain,” Nature, vol. 65… · 2026
[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
rf quantum capacitance (parity) · 100 µs · non-destructive · mid-circuit
(d) mobility
—
(e) control
low-frequency electrical @ room temperature
(f) error structure
unknown / contested
(g) manufacturing
III-V MBE heterostructures

Evaluation space — dated attributes

readout → 1% error; SNR 1 in 3.6 µs
defines: clock (cycle time) · 2025-02 · source
independent replication (QuTech, InSb Kitaev chain) → ~1.85 ms dwell, SNR ~1.93
defines: clock (cycle time) · 2026-02 · source

The independent replication is van Loo et al., Nature 650 (2026-02-11), on an InSb minimal Kitaev chain; arXiv:2607.09511 is the follow-on coherent parity qubit, a different result.

Standard records

reset / initialisation time → not published · typical
No initialisation or reset procedure is described for the tetron parity readout · 2025-02 · source [D] ⓘ
reset error → not published · typical
No reset error published, because no reset is demonstrated · 2025-02 · source [D] ⓘ
SPAM error → 0.01 · typical
Microsoft tetron: 'a parity measurement with an assignment error probability of 1%'; SNR 1 in 3.6 us · 2025-02 · source [D] ⓘ
QND fidelity / survival → not published · typical
QND-ness is not quantified; the paper gives parity dwell times >1 ms and tau_RTS ~ 2 ms (quasiparticle poisoning) · 2025-02 · source [D] ⓘ

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: Minimal Kitaev chain and parity measurement setup. a, Illustration of a global parity measurement, coupling simultaneously to both Majoran…
Seven-panel paper figure: cartoons and energy diagrams of a minimal Kitaev chain (two quantum dots joined by a superconducting segment) and its even and odd parity states, a parity map, a real false-coloured scanning-electron micrograph of the device (200 nm scale bar), and a readout circuit schematic. From the arXiv paper "Single-shot parity readout of a minimal Kitaev chain" by Nick van Loo and co-authors. It shows why a measurement must couple to both Majorana modes at once to tell the parity states apart, here read out by radio-frequency reflectometry. “Fig. 1 — Figure 1: Minimal Kitaev chain and parity measurement setup. a, Illustration of a global parity measurement, coupling simultaneously to both Majorana zero…” by Nick van Loo et al., arxiv.org/abs/2507.01606, CC BY 4.0 (creativecommons.org/licenses/by/4.0/)
Fig. 4 — Figure 4: Local and global probes of parity switching. a, Schematic of the dual readout setup: global parity is detected via quantum capacitance Δ​S…
A cartoon plus measured time traces. (a) Two quantum dots hosting Majorana modes γ1 and γ2, watched by a global probe (quantum capacitance) and a local one (charge sensing); (b) at the sweet spot the quantum-capacitance signal jumps between two levels as the chain's parity switches, while the charge sensor sees only noise; (c) a map of the correlation between both signals versus two gate voltages; (d), (e) away from the sweet spot both signals switch together, positively or negatively correlated. It comes from van Loo, Zatelli, Steffensen and co-authors, 'Single-shot parity readout of a minimal Kitaev chain'. Majorana-based topological qubits rely on such non-locally stored parity. “Fig. 4 — Figure 4: Local and global probes of parity switching. a, Schematic of the dual readout setup: global parity is detected via quantum capacitance Δ​SM11…” by Nick van Loo et al., arxiv.org/abs/2507.01606, CC BY 4.0 (creativecommons.org/licenses/by/4.0/)
Fig. 1 — Figure 1: (a) Electronic and cryogenic setup. An RF tone PinP is split in two at room temperature (RT). One part serves as local oscillator (LO) for
Three-panel figure. (a) A drawing of the measurement chain from room temperature through 4 K to 50 mK: attenuated input and pump lines, a directional coupler, isolators, a Josephson travelling-wave parametric amplifier (+12 dB), a high-electron-mobility-transistor (HEMT) amplifier (+35 dB) and an IQ demodulator, with an optical micrograph of the spiral inductor forming the tank circuit on gate B3. (b) A false-coloured scanning electron micrograph of a four-dot silicon (SiMOS) device with gates B1–B3 and T1–T3. (c) A charge-stability map of the demodulated signal. It is Fig. 1 of arXiv 2307.14717 by V. Elhomsy and co-authors. It shows where a parametric amplifier sits in gate-based spin-qubit readout. “Fig. 1 — Figure 1: (a) Electronic and cryogenic setup. An RF tone PinP is split in two at room temperature (RT). One part serves as local oscillator (LO)…” by Victor Elhomsy et al., arxiv.org/abs/2307.14717, CC BY 4.0 (creativecommons.org/licenses/by/4.0/)
ro_qcap · layer 6 Readout · centrality 5.7 · emerging · since 2025 · updated 2026-09-04

rf quantum-capacitance parity readout

Dispersive gate sensing of a Majorana island's quantum capacitance by rf reflectometry, reading fermion parity without charge transfer; non-destructive and mid-circuit.

Verdict. The method is real and independently replicated; falsified as fault-tolerance-grade unless an assignment error below 10⁻³ at a stated integration time is published by 2028, on any stack.

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 dot–nanowire interference loop's ground state disperses differently with gate charge in the two parity sectors; that curvature is a quantum capacitance, read as a dispersive shift of an off-chip resonator by rf reflectometry, with no charge transfer. Microsoft, Nature 2025-02-19: 1% assignment error, SNR 1 in 3.6 µs, dwell above 1 ms near 2 T D[13]. This is the single-wire (Z-type) measurement; the joint projection a gate needs is unbuilt.
a fabricated (1.0) · b not a gate · c quantum capacitance, ~4 µs, non-destructive, mid-circuit
d no transport · e rf reflectometry from room temperature · f assignment error plus poisoning · g MBE wire stack

Physics & limits

Signal accumulates as √t while parity survives only until a quasiparticle arrives, so assignment error is a race, modelled as err ≈ ½[1 − e^(−2t/τ)·erf(SNR/√2)²] at mean SNR near 1.2 per µs D[20]. The floor is the poisoning time τ, set by loop geometry, not the amplifier: the same device gives 12.4 ms on the Z loop against 14.5 µs on the X loop, attributed to the two-loop configuration's larger quasiparticle-capture cross-section D[20]. Lead replaced aluminium to raise τ D[21]. What it reads is contested: Nature's editor's note says the results do not by themselves establish Majorana zero modes P[214].

Engineering state of the art

table
Year Figure Who Tag+key
2025-02 1% assignment error, SNR 1 in 3.6 µs, dwell >1 ms, InAs–Al Microsoft Azure Quantum D[13]
2026-02 Independent single-shot parity readout, ~1.85 ms switching, InSb Kitaev chain QuTech D[216]
2026-06 ~20 s parity switching in one InAs–Pb wire, same readout family Microsoft Quantum D[21]

Typical at scale is undefined: no multiplexed multi-tetron readout is published; the 2026 device came up one wire at a time D[21].

The arXiv full text of [20] also gives X ~4 µs and Z ~9.3 ms for other tunings, against the 14.5 µs / 12.4 ms used here. The quasiparticle-poisoning rate during a readout dwell has only been inferred, never measured directly. Not published: a readout-specific R&D spend.

Manufacturing, materials & supply chain

No dedicated process: dots, gates and loop share the wire device's lithography, resonator off-chip. Room-temperature rf drive and demodulation feed a millikelvin amplifier, from the merchant control-electronics base superconducting readout uses Cfact; no single point of failure beyond the wire stack, and no export-control category specific to it. I/O is a gate line and a resonator per measurable parity, multiplexed on a shared feedline: 10³ is solved packaging. The wall is time: 3.6 µs is fast against 12.4 ms, slow against 14.5 µs, so at 10⁴–10⁶ the limit is how many X projections fit in the shorter window.

Role in the stack

The one demonstrated block the topological architecture owns: it requires the Majorana-parity carrier and provides the projective measurement a measurement-based gate would consume, non-destructively and mid-circuit, the precondition for measurement-only architecture. It is the only defined term of the architecture's derived clock: in sum of the syndrome round: gate layers + transport + readout + reset only readout is published, ~3.6 µs to SNR 1 D[13], with no code and no reset figure. Verification: QuTech's Nature paper (2026-02-11) independently replicates the principle on InSb dot-based Kitaev chains rather than a tetron, at ~1.85 ms telegraph lifetimes D[216]; its follow-up shows coherent parity oscillations with only limited protection D[217]. Legg disputes whether the read regions are gapped at all D[22]. Nobody has replicated the 1% error.

Actors & economics

Who.
| Organisation | Role | Country | What they do | Evidence |
|---|---|---|---|---|
| Microsoft Quantum | developer | US | Originated the method; used on every tetron device | D[13] |
| QuTech | research | NL | Independent parity readout and coherent parity qubit, on Eindhoven-grown InSb wires | D[216] |
| DARPA | investor | US | Funds the only industrial user; US2QC final stage since 2025-02-06 | fact |

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

Market & supply chain. No standalone market; rf reflectometry and cryogenic amplification are generic and multi-sourced, so concentration risk sits in the wire stack. G3 and G4 only.

IP & standards. Dispersive gate sensing is common property across semiconductor-qubit groups; no dated patent count specific to parity readout as of 4 Sep 2026.

Roadmaps & track record. (used in every public Microsoft device from 2025-02, implicitly for fault tolerance by 2029; status 4 Sep 2026: no fidelity or speed target published for the readout) C[215]. QuTech publishes with no schedule to defend, the more credible record.

Strategic reading. The method is public and replicated, so Microsoft's exclusivity has moved into the wire stack; whoever first publishes assignment error near 10⁻³ at a stated integration time sets the downstream pace.

Outlook & open questions

Falsifiable in 12–24 months: a third group publishing parity readout; a sub-1% assignment error from anyone but Microsoft; a directly measured poisoning rate. Confirm if two land; demote if it stays a two-laboratory result to 2028. Best case, readout stops being the open variable; worst case, τ on a joint loop stays in tens of µs. Open: does multiplexed multi-tetron readout work; is 1% reproducible off Microsoft's devices.

References
  1. [13] Microsoft Azure Quantum, “Interferometric single-shot parity measurement in InAs–Al hybrid devices,” Nature, vol. 638, no. 8051, pp. 651–655, Feb. 2025, doi: 10.1038/s41586-024-08445-2. D
  2. [20] M. Aghaee et al., “Distinct Lifetimes for X and Z Loop Measurements in a Majorana Tetron Device,” arXiv:2507.08795, Jul. 2025. D
  3. [21] M. Aghaee et al., “20 Second Parity Lifetime in an InAs–Pb Tetron Device,” arXiv:2606.03884, Jun. 2026. D
  4. [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
  5. [214] P. Ball, “Experts Weigh in on Microsoft's Topological Qubit Claim,” Physics, vol. 18, p. 57, 2025. [Online]. Available: https://physics.aps.org/articles/v18/57 P
  6. [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
  7. [216] N. van Loo et al., “Single-shot parity readout of a minimal Kitaev chain,” Nature, vol. 650, no. 8101, pp. 334–339, Feb. 2026, doi: 10.1038/s41586-025-09927-7. D
  8. [217] F. Zatelli et al., “Majorana parity qubit in coupled minimal Kitaev chains,” arXiv:2607.09511, Jul. 2026. D