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III-V MBE heterostructures (InAs–Pb wires, QD sources) fab_mbe

Molecular beam epitaxy of III-V nanostructures with vacuum-unbroken superconductor shells for Majorana wires, and of quantum dots for single-photon sources.

III-V MBE heterostructures (InAs–Pb wires, QD sources)

fab_mbe · layer 10 Manufacturing · demonstrated · since 2015

In-house Microsoft growth for tetrons (no external replication); GaAs quantum-dot photon sources (Quandela).

Brief →

Key references

[21] M. Aghaee et al., “20 Second Parity Lifetime in an InAs–Pb Tetron Device,” arXiv:2606.0388… · 2026
[365] H. Zhang et al., “Quantized Majorana conductance,” Nature, vol. 556, no. 7699, pp. 74–79, … · 2018
[13] Microsoft Azure Quantum, “Interferometric single-shot parity measurement in InAs–Al hybrid… · 2025
[22] H. F. Legg, “On the robustness of topological gap detection via transport,” Nature, vol. 6… · 2026
[301] US Department of Commerce, Bureau of Industry and Security, “Commerce Control List Additio… · 2024

Design space — attributes

(a) carrier affinity
hybrid (fabricated host)
(b) time · entangling
—
(c) readout
—
(d) mobility
—
(e) control
—
(f) error structure
unknown / contested
(g) manufacturing
III-V MBE heterostructures

Evaluation space — dated attributes

replication → no independent replication of the InAs–Pb stack
defines: scaling path · 2026-06 · source

Lead against aluminium in Microsoft's stacks: the superconductor's own gap ≈1.3 meV vs 295 µeV and the induced gap ≈570 vs 129 µeV, each about fourfold; the top-quintile topological gap ~70 vs ~30 µeV, about twofold (tetron preprint, 2026; PRB 107, 245423). The lineage starts with in-situ epitaxial Al on InAs nanowires (Copenhagen, 2015); the 2018 quantised-Majorana-conductance claim, made on InSb–Al wires (Nature 556), was retracted on 2021-03-08. MBE growth equipment is export-controlled under ECCN 3B001.a.3; the 2024 rule's 3C907 covers only epitaxy of isotopically enriched Si or Ge. QuTech's InSb wires are grown at TU Eindhoven (Bakkers).

Standard records

device yield → not published · typical
No device yield: Microsoft says only that 'several devices, fabricated according to the design's engineering specifications, have passed' · 2022-07 · source [D] ⓘ
parameter spread → not published · typical
No wafer-level parameter spread published for the InAs-Al or InAs-Pb heterostructures; only per-device topological gaps are quoted: maxima of 20–60 µeV for InAs-Al, a top-quintile ~70 µeV for InAs-Pb (against ~30 µeV for InAs-Al on that measure; tetron preprint arXiv:2606.03884, 2026) · 2022-07 · source [D] ⓘ

Actors & goals — annotations

Fusion-based photonic (FBQC) (alternate) — PsiQuantum (Omega), Quandela, QuiX · G4 G6

Edges

needed by: Majorana parity (InAs–Pb tetron), Single photon (discrete variable)°
° one of several that would do · the usual route, not a strict need

Used by 4 machines (2 primary · 2 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.

File:Molecular-beam epitaxy 412 RIBER system at LAAS-CNRS.jpg
A photograph of a complete molecular beam epitaxy system in a clean room: a gold-coloured RIBER growth chamber with radial source-cell ports, a grey insulated preparation chamber and load-lock modules on blue frames. Taken by QGravelier on 22 June 2021 at the LAAS-CNRS technology facility in Toulouse, France; the file title names it a RIBER 412 system. It is fabrication equipment, not a quantum computer, but shows the scale of the ultra-high-vacuum tools that grow III-V heterostructures for nanowire and quantum-dot devices. “Molecular-beam epitaxy 412 RIBER system at LAAS-CNRS” by QGravelier, commons.wikimedia.org/wiki/File:Molecular-beam_epitaxy_412_R…, CC BY SA 4.0 (creativecommons.org/licenses/by-sa/4.0/)
File:MBE.svg
Labelled drawing, not a photograph, of the inside of a molecular-beam-epitaxy chamber: heated effusion cells send beams of material onto a rotating, heated substrate, while cryopanels, a RHEED electron gun and screen, a mass spectrometer and gauges monitor the growth. It is a concept drawing by Vegar Ottesen dated 2011-10-11 (origin as recorded: Wikimedia Commons). It explains how the III-V layers behind quantum-dot photon sources and hybrid nanowires are grown one atomic layer at a time. “MBE” by Vegar Ottesen, commons.wikimedia.org/wiki/File:MBE.svg, CC BY 3.0 (creativecommons.org/licenses/by/3.0/)
File:Molecular-beam epitaxy system at LAAS 0513.jpg
A photograph of the growth chamber of a molecular beam epitaxy machine: a gold-coloured, RIBER-labelled vessel with bolted flanges and windows, its source ports wrapped in aluminium foil, next to a load-lock box marked 'LOAD'. The caption places it at the LAAS-CNRS facility in Toulouse, photographed by Guillaume Paumier in October 2007. Inside such a chamber, heated cells send atomic beams onto a wafer to build III-V semiconductor layers; the foil is typical of bakeout to reach ultra-high vacuum. “Molecular-beam epitaxy system at LAAS 0513” by Guillaume Paumier (user:guillom), commons.wikimedia.org/wiki/File:Molecular-beam_epitaxy_syste…, CC BY SA 3.0 (creativecommons.org/licenses/by-sa/3.0)
fab_mbe · layer 10 Manufacturing · centrality 4.2 · demonstrated · since 2015 · updated 2026-09-30

III-V MBE heterostructures (InAs–Pb wires, QD sources)

Molecular beam epitaxy of III-V nanostructures with vacuum-unbroken superconductor shells for Majorana wires, and of quantum dots for single-photon sources.

Verdict. The process works and is single-source; falsified as a reproducible platform unless a group outside Microsoft publishes an independently grown InAs–Pb device with comparable parity signatures 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

Two unrelated devices share a tool class. The first is a III-V nanowire or 2DEG (two-dimensional electron gas) grown by molecular beam epitaxy (MBE) with a superconductor deposited in the same vacuum, so the interface is never exposed: aluminium through 2025, lead in the 2026 tetron as the higher-gap shell D[21]. The second is GaAs-based quantum dots as single-photon sources, same reactors, different physics fact. The lineage dates to 2015, when Copenhagen grew aluminium epitaxially on InAs nanowires without breaking vacuum Dfact; the field's 2018 headline, quantised Majorana conductance in InSb–Al wires, was retracted on 2021-03-08 D[365].
a mostly fabricated (0.75) · b a process, not a clock · c none · d none
e none · f disorder-dominated · g molecular beam epitaxy

Physics & limits

The floor is disorder. Unintentional doping, interface roughness and shell strain produce trivial sub-gap Andreev states whose signatures mimic Majorana zero modes (MZMs), which is the Nature dispute: Legg argues the regions used for parity readout are disordered and gapless D[22]. Lead raises the gaps above aluminium's: in Microsoft's tetron stack the lead film's own gap is ≈1.3 meV and the gap it induces in the wire ≈570 µeV, against 295 µeV and 129 µeV with aluminium, while the topological gap, taken at the top quintile of its measured values, only doubles, from ~30 to ~70 µeV D[21], fact; epitaxial Pb on InAs nanowires holds a hard 1.25 meV gap to 8.5 T (Copenhagen, 2021) Dfact. Moving the floor means a mean free path well above the coherence length, verified by a published mobility or disorder metric rather than device outcomes. Microsoft published such metrics for InAs–Al — mobility 60,000–100,000 cm²/V·s, a charged-defect density of 2.7 × 10¹² cm⁻² Dfact — and for the Pb stack only Hall-bar values of its active region, a surface charge density of ≈2 × 10¹² cm⁻² and a buried-well mobility above 350,000 cm²/V·s D[21]; none is measured on a device, which is why the materials argument runs through transport data.

Engineering state of the art

table
Year Figure Who Tag+key
2018 Quantised-conductance Majorana claim in InSb–Al wires; retracted 2021-03-08 Delft (Kouwenhoven et al.) D[365]
2025-02 InAs–Al stack supports 1% parity assignment error Microsoft Azure Quantum D[13]
2026-06 InAs–Pb stack, higher-gap shell, ~20 s parity switching, one wire Microsoft Quantum D[21]

No yield or uniformity figure is published for either stack, and the Pb one's disorder figures come from Hall bars, not devices; the only public scaling aid is an rf method resolving wire-end-state splitting to µeV for per-device bring-up D[21].

For InAs–Al, Microsoft published an induced gap of 129 µeV, topological gaps of 20–60 µeV, a mobility and a charged-defect density (Physical Review B, 2023) fact, from a gap protocol whose reading Legg disputes D[22]; for the InAs–Pb stack the tetron paper gives the lead film's gap (≈1.3 meV), the induced gap (≈570 µeV), a top-quintile topological gap (~70 µeV) and Hall-bar charge density and mobility [21]. ECCN 3C907 covers only silicon or germanium with an isotopic impurity below 0.08% G[301]; whether a given III-V stack falls under 3C001.d depends on its layers and doping, and no BIS ruling addresses it. Not published: a yield metric for either stack, and a dated revenue or market-share figure for merchant MBE tool vendors.

Manufacturing, materials & supply chain

Growth needs a III-V MBE reactor under ultra-high vacuum with in-situ superconductor deposition, keeping the interface clean enough for a hard gap. Microsoft's recipe is in-house, and since 2025-11-13 the full Majorana chip core is fabricated at Lyngby in Denmark Pfact; nobody outside has grown an equivalent stack, so one recipe in one building is the architecture's single point of failure D[22]. An independent III-V base exists for another geometry: Eindhoven-grown InSb wires carry QuTech's Kitaev devices D[216]. Export exposure predates the quantum rules: MBE growth equipment has long been on the Wassenaar dual-use list (US Export Control Classification Number 3B001.a.3), and a III-V hetero-epitaxial wafer falls, if anywhere, under 3C001.d fact; the BIS rule of 2024-09-06 added 3C907 only for epitaxial layers of isotopically enriched silicon or germanium, which leaves an InAs–Pb stack outside it G[301]P[818].

Role in the stack

Everything in the topological architecture stands on this stack: encoding, readout and the unbuilt gate inherit its disorder. It provides no clock and no fidelity, only the ceiling on everyone else's; its one load-bearing fact is negative: no independent replication D[22]. The same tool class supplies quantum-dot single-photon sources to the fusion-based photonic architecture fact. The register lists four machines using it, among them Lucy, Belenos, Majorana 1 and Majorana 2. Verification here is materials verification and does not exist: the Nature exchange of 2026-06-24 disputes transport data from one laboratory's wafers, Microsoft conceding nothing D[22]; no second laboratory has grown the planar Pb stack, though Copenhagen put epitaxial Pb on InAs nanowires in 2021 Dfact.

Actors & economics

Who.
| Organisation | Role | Country | What they do | Evidence |
|---|---|---|---|---|
| Microsoft Quantum | developer | US | Grows and consumes the InAs–Pb stack; fab in Lyngby | Pfact |
| DARPA | investor | US | Funds both users: US2QC final stage, QBIT Stage A | fact |

Money. 2025-02-06 · Microsoft · US2QC enters its final stage · undisclosed · DARPA · announced fact. 2025-11-13 · Microsoft · Lyngby (DK) Majorana chip-core fab · >DKK 1 bn national total, Microsoft's outlay undisclosed · announced Pfact. 2026-06-16 · Quandela · DARPA QBIT Stage A selection · announced fact.

Market & supply chain. MBE reactors are a small merchant market, but the tool is not the bottleneck: the recipe is, and it is not for sale. G3/G4 pay for the wires, G6 for the photon sources.

IP & standards. No dated patent count specific to this process as of 4 Sep 2026; no standard covers these interfaces.

Roadmaps & track record. (three wire generations, InSb–Al 2018 → InAs–Al 2025 → InAs–Pb 2026, promised as the base for fault tolerance by 2029; status 4 Sep 2026: materials delivered, no yield metric published) C[215]. Lyngby opened as announced; the retracted 2018 result is why outsiders discount later ones.

Strategic reading. While the recipe stays secret every claim above it is unfalsifiable from outside; independent replication either way is worth more than another Microsoft device. Success means a stack nobody can second-source; failure moves value to the InSb base.

Outlook & open questions

Falsifiable in 12–24 months: an outside lab publishing an independently grown planar InAs–Pb device with parity readout; a published yield, or a disorder metric measured on Microsoft's Pb devices rather than Hall bars. Confirm on the first; without it the dispute is unresolvable. Best case, an academic group reproduces the stack; worst case, the recipe stays proprietary and the architecture unauditable to 2029. Open: the spread of topological gaps behind the top-quintile ~70 µeV; yield per wafer; whether anyone outside Microsoft grows the planar Pb stack.

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. [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. [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
  6. [301] US Department of Commerce, Bureau of Industry and Security, “Commerce Control List Additions and Revisions; Implementation of Controls on Advanced Technologies Consistent With Controls Implemented by International Partners,” Federal Register, vol. 89, p. 72926, Sep. 6, 2024. [Online]. Available: https://www.federalregister.gov/documents/2024/09/06/2024-19633/commerce-control-list-additions-and-revisions-implementation-of-controls-on-advanced-technologies G
  7. [365] H. Zhang et al., “Quantized Majorana conductance,” Nature, vol. 556, no. 7699, pp. 74–79, Mar. 2018, doi: 10.1038/nature26142. Retracted: Nature, vol. 591, p. E30, Mar. 2021, doi: 10.1038/s41586-021-03373-x. D
  8. [818] J. P. Barker et al., “Commerce Implements Export Controls on Semiconductor, Additive Manufacturing, and Quantum Computing Items,” Arnold & Porter, Sep. 10, 2024. [Online]. Available: https://www.arnoldporter.com/en/perspectives/advisories/2024/09/semiconductor-additive-manufacturing-and-quantum-computing P