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CV Gaussian gates + GKP-assisted non-Gaussian operations g_cv

Beamsplitters, squeezers and homodyne feed-forward on optical modes, with GKP grid states supplying the non-Gaussian resource fault tolerance requires.

CV Gaussian gates + GKP-assisted non-Gaussian operations

g_cv · layer 3 Gate mechanism · demonstrated · since 2020

Beamsplitters, squeezers and homodyne feed-forward on optical modes at 1 MHz clock (Aurora).

Brief →

Key references

[413] D. Gottesman, A. Kitaev, and J. Preskill, “Encoding a qubit in an oscillator,” Phys. Rev. … · 2001
[821] S. Yokoyama et al., “Ultra-large-scale continuous-variable cluster states multiplexed in t… · 2013
[173] H. A. Rad et al., “Scaling and networking a modular photonic quantum computer,” Nature, vo… · 2025
[174] M. V. Larsen et al., “Integrated photonic source of Gottesman–Kitaev–Preskill qubits,” Nat… · 2025
[642] Xanadu, “Xanadu Unveils 1st On-Chip Error-Resistant Photonic Qubit,” HPCwire, Jun. 5, 2025… · 2025

Design space — attributes

(a) carrier affinity
photon (natural particle, engineered modes)
(b) time · entangling
1.0 µs · deterministic
(c) readout
—
(d) mobility
flying qubits (photons)
(e) control
electro-optic @ room temperature
(f) error structure
Gaussian (small-shift), loss (erasure)
(g) manufacturing
photonic IC foundry

Evaluation space — dated attributes

Aurora clock → 1 MHz, 12 modes per cycle
defines: clock (cycle time) · 2025-01 · source

Time-domain-multiplexed CV cluster states originate with Yokoyama et al. (University of Tokyo, 2013, > 10,000 modes); Xanadu's Aurora is the first modular chip-based networked version, not the first such state.

Standard records

1Q gate time → 1.0 µs · typical
Xanadu Aurora: 1 MHz clock with 12 physical qubit modes per cycle - 1 us per Gaussian-gate cycle; 7.2e9 temporal modes · 2025-01 · source [D] ⓘ
2Q error under full-width parallel operation → not published · typical
No error-per-gate is defined for CV two-mode operations; Aurora is characterised by loss (>95% on heralded paths) and squeezing · 2025-01 · source [D] ⓘ
crosstalk → not published · typical
No crosstalk figure: mode mixing in a CV interferometer is the programmed operation, not an error channel · 2025-01 · source [D] ⓘ

Actors & goals — annotations

Edges

needs: Squeezed light mode (CV), Electro-optic drive + feed-forward electronics (room temperature)
alternatives: Linear-optical fusion (heralded)
° one of several that would do · the usual route, not a strict need

Used by 3 machines (1 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.

Fig. 1 — Figure 1: Conceptual diagram and experimental procedure for simulating the advection equation on a continuous-variable quantum platform. (A) The cla…
A two-part concept drawing, not a picture of the apparatus. (A) The advection equation, which carries a quantity along d coordinates, is mapped onto continuous-variable (CV) light: x becomes the x̂ quadrature, ∂/∂x becomes ip̂, and each coordinate becomes a separate light pulse in time. (B) The workflow: one-mode squeezed, two-mode squeezed or multi-mode cluster-state pulses each receive a displacement, homodyne detection samples their quadratures, then statistics follow. It is Figure 1 of arXiv 2606.00581, 'Analog photonic simulator for large-scale transport' (Zhao, Su and co-authors). Notice why it works: a Hamiltonian linear in p̂ just displaces each pulse, so advection needs only displacements, a Gaussian operation. “Fig. 1 — Figure 1: Conceptual diagram and experimental procedure for simulating the advection equation on a continuous-variable quantum platform. (A) The classical…” by Mengyu Zhao et al., arxiv.org/abs/2606.00581, CC BY 4.0 (creativecommons.org/licenses/by/4.0/)
Fig. 3 — Figure 3: Characteristics of MBQC on noisy GKP cluster states (a) A GKP wave function at squeezing rate sgkp=12s=12 dB. As one decreases the squeez
A three-panel figure of computed plots: a Gottesman-Kitaev-Preskill (GKP) wavefunction drawn as a comb of peaks, gate infidelity versus squeezing, and maps of quantum volume versus squeezing and optical transmission. It is Figure 3 of the arXiv paper "Quantum Volume for Photonic Quantum Processors" by Yuxuan Zhang and co-authors. It shows what measurement-based computing on GKP cluster states needs: with weaker squeezing the red and blue peaks overlap, causing logical errors, and the grey band marks transmission too low for log2(QV) of 10 even with ideal squeezing. “Fig. 3 — Figure 3: Characteristics of MBQC on noisy GKP cluster states (a) A GKP wave function at squeezing rate sgkp=12s=12 dB. As one decreases the…” by Yuxuan Zhang, Daoheng Niu, Alireza Shabani, Hassan Shapourian, arxiv.org/abs/2208.11724, CC BY 4.0 (creativecommons.org/licenses/by/4.0/)
Fig. 2 — Figure 2: Cubic phase gate and non-Gaussian states. (a) The potential and (b) the pointwise force. Target: the programmed potential. Sim: the finite…
A figure of plots, not a device image. (a) The programmed cubic potential V(X) and (b) its force V′(X), each showing target, simulation and experiment; (c) for three coherent input states, the measured characteristic function (real and imaginary parts) and the reconstructed Wigner function, with fidelities 0.84–0.90. It is Fig. 2 of arXiv 2609.02405 (September 2026) by Clara Yun Fontaine, … Yvonne Y. Gao, on programming anharmonic potentials in a superconducting harmonic oscillator. The cubic phase gate is the standard non-Gaussian gate for continuous-variable quantum computing, here made with qubit-conditioned displacements on a superconducting oscillator rather than light; notice the crescent-shaped Wigner functions with negative (blue) regions. “Fig. 2 — Figure 2: Cubic phase gate and non-Gaussian states. (a) The potential and (b) the pointwise force. Target: the programmed potential. Sim: the finite-order…” by Clara Yun Fontaine et al., arxiv.org/abs/2609.02405, CC BY 4.0 (creativecommons.org/licenses/by/4.0/)
g_cv · layer 3 Gate mechanism · centrality 4.2 · demonstrated · since 2020 · updated 2026-09-03

CV Gaussian gates + GKP-assisted non-Gaussian operations

Beamsplitters, squeezers and homodyne feed-forward on optical modes, with GKP grid states supplying the non-Gaussian resource fault tolerance requires.

Verdict. On-chip GKP effective squeezing is 0.62 dB against the ~10 dB the architecture needs — an ~8.7× grid-noise-variance gap. If Xanadu's 2028–29 fault-tolerance milestone slips, this is the slowest photonic track.

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

Gates act on optical quadratures — beamsplitters, phase shifts, squeezers — closed by homodyne feed-forward. Gaussian operations with homodyne detection are classically simulable, so universality needs a non-Gaussian resource: the Gottesman–Kitaev–Preskill grid state, 2001 S[413]. Time-domain multiplexing predates the companies — the University of Tokyo entangled over 10,000 modes in 2013 D[821]; Xanadu added the modular chip version D[173] and the first integrated GKP source D[174]. Attributes: flying carrier, partly fabricated, ~1 µs deterministic step, Gaussian-noise and loss-dominated error; electro-optic control at room temperature, photonic-IC fabrication.

Physics & limits

Loss acts as a Gaussian random-displacement channel on the grid, blurring the GKP peaks until modular-quadrature measurement cannot resolve the logical value; the floor is effective squeezing, not gate count. Xanadu's on-chip source reports 0.62 dB D[174] — grid-noise variance ~0.87 of vacuum against ~0.10 at the ~10 dB assumed, an ~8.7× reduction still to find S, a different quantity from Xanadu's 24.1× loss factor above threshold C[178]. Only lower per-element loss, better sources and deeper multiplexing move it. Feed-forward adds a second floor: electronics must act inside the ~1 µs clock, and the published CV loop is 196 ns P[822].

Engineering state of the art

table
Date Figure Who Tag
2013-11 >10,000-mode time-domain CV cluster state Univ. of Tokyo D[821]
2025-01 Aurora: 35 chips, 12 modes per 1 MHz cycle, 2 h, ~14 dB loss Xanadu D[173]
2025-06-05 First integrated GKP source, 0.62 dB effective squeezing, SiN Xanadu D[174]

No GKP logical qubit exists; Aurora ran two hours without error correction and reported no logical fidelity, so it shows stability, not computation D[173].

The date, platform and room-temperature operation of the 0.62 dB GKP result come from the publisher's press coverage [642], and no independent group has replicated it. Published GKP threshold estimates vary with decoder and architecture, so the ~10 dB figure is not a single authoritative value. The 0.87→0.10 variance conversion is derived, not quoted. Xanadu's 24.1× loss factor and the 0.62 dB effective squeezing are different quantities that no source reconciles.

Manufacturing, materials & supply chain

Fabrication is silicon-nitride lithography on 300 mm-class wafers, shared with the discrete-variable sector; the CV-specific additions are squeezers and high-efficiency homodyne receivers rather than switches, and the GKP source runs at room temperature D[174]. Packaging is Corning fibre arrays and DISCO singulation C[172]. Control is the heavy part: every mode needs a homodyne receiver, an ADC and a loop closing inside the clock, scaling linearly with no published shortcut. At 10³ modes that is a rack of receivers, at 10⁴ the analogue front end dominates, and nothing addresses 10⁶. ECCN 4A906 applies to the machine fact.

Role in the stack

The continuous-variable architecture's gate layer, requiring squeezed sources and room-temperature feed-forward. It substitutes for rather than complements discrete-variable fusion: CV measures quadratures where fusion detects single photons, so switching architectures replaces sources, detectors and decoders together. Derived clock 1.0 MHz D[173]. Verification is thin: the 0.62 dB is single-group, unreplicated, and routinely confused with raw quadrature squeezing — the 1.4 dB in periodically poled TFLN P[345] is a different quantity.

Actors & economics

Who.
Organisation Role Country What they do Evidence
Xanadu developer CA Aurora, integrated GKP source, GKP+qLDPC roadmap D[173]D[174]
University of Tokyo research JP Origin of large-scale time-domain CV cluster states D[821]
Corning supplier US Fibre arrays behind Xanadu's coupling figure C[172]

Money.
2025-11-06 · Xanadu · DARPA QBI Stage B selection · up to USD 15 M · DARPA · announced fact
2026-03-26 · Xanadu · SPAC merger with Crane Harbor · ~USD 302 M gross, ~40% below plan · closed Cfact
2026-08-28 · Xanadu · Toronto factory funding · CAD 195 M · Government of Canada · announced C[178]
2026-08-31 · Xanadu · liquidity · ~USD 686 M at 2026-06-30 · reported Cfact

Market & supply chain. One commercial actor, so no market — only Xanadu's supply relationships and the packaging concentration it shares with photonics generally. CV pays for G1 today; G3/G4 only if squeezing closes, G6 the natural adjacency.

IP & standards. No dated CV/GKP patent count from a named database as of 2026-09-04; Strawberry Fields/Blackbird is the only CV-native open-source stack, used by no other vendor.

Roadmaps & track record. The 2026-08-31 release is Xanadu's first quantified schedule (promised 2026-08: fault tolerance 2028–29, 200 logical qubits 2029, 1,000+ by 2031) — too new to score C[178]; against it stands one miss, the SPAC closing ~40% below plan Cfact. Its physics claims are self-critical; its financing claims are not.

Strategic reading. If effective squeezing improves an order of magnitude, CV's flying room-temperature carrier is the natural networking substrate and G6 is Xanadu's to lose. If not, no second actor exists to inherit the track, and its suppliers are worth more than its architecture.

Outlook & open questions

Confirm by 2027: effective squeezing above 3 dB on chip; demote the 2028–29 milestone if it stays below 1 dB. Best case 2029: a small GKP logical qubit at low distance. Worst case: uncorrected demonstrations continue and the schedule slips as the financing did. Open: how much of the gap is loss versus fabrication; do homodyne front-ends scale.

References
  1. [172] Xanadu, “Xanadu sets new industry benchmark in photonic chip packaging,” PR Newswire, Jun. 10, 2026. [Online]. Available: https://www.prnewswire.com/news-releases/xanadu-sets-new-industry-benchmark-in-photonic-chip-packaging-302796562.html C
  2. [173] H. A. Rad et al., “Scaling and networking a modular photonic quantum computer,” Nature, vol. 638, no. 8052, pp. 912–919, Jan. 2025, doi: 10.1038/s41586-024-08406-9. D
  3. [174] M. V. Larsen et al., “Integrated photonic source of Gottesman–Kitaev–Preskill qubits,” Nature, vol. 642, no. 8068, pp. 587–591, Jun. 2025, doi: 10.1038/s41586-025-09044-5. D
  4. [178] Xanadu Quantum Technologies Limited, “Xanadu Charts Path to Over 1,000 Logical Qubits by 2031,” GlobeNewswire, Aug. 31, 2026. [Online]. Available: https://www.globenewswire.com/news-release/2026/08/31/3353211/0/en/xanadu-charts-path-to-over-1-000-logical-qubits-by-2031.html C
  5. [345] X. Shi et al., “Squeezed Light Generation in Periodically Poled Thin-Film Lithium Niobate Waveguides,” arXiv:2508.08599, Aug. 2025. P
  6. [413] D. Gottesman, A. Kitaev, and J. Preskill, “Encoding a qubit in an oscillator,” Phys. Rev. A, vol. 64, no. 1, Art. no. 012310, Jun. 2001, doi: 10.1103/PhysRevA.64.012310. arXiv:quant-ph/0008040. S
  7. [642] Xanadu, “Xanadu Unveils 1st On-Chip Error-Resistant Photonic Qubit,” HPCwire, Jun. 5, 2025. [Online]. Available: https://www.hpcwire.com/off-the-wire/xanadu-unveils-1st-on-chip-error-resistant-photonic-qubit/ P
  8. [821] S. Yokoyama et al., “Ultra-large-scale continuous-variable cluster states multiplexed in the time domain,” Nat. Photon., vol. 7, no. 12, pp. 982–986, Dec. 2013, doi: 10.1038/nphoton.2013.287. D
  9. [822] D. Duggan et al., “FPGA Based Feedforward System for Photonic Quantum Computing Applications,” arXiv:2606.03500, Jun. 2026. P