← Quantum Technology AtlasTechnologies · Machines · Architectures · OrganisationsРусскийעברית

Ion-chain motional bus (all-to-all in chain) cx_bus

A shared collective motional mode entangles any pair in one trap, giving genuine all-to-all connectivity at the price of gate time growing with chain length.

Ion-chain motional bus (all-to-all in chain)

cx_bus · layer 4 Connectivity / transport · demonstrated · since 2003

Shared motional modes give all-to-all within one chain; gates slow with chain length (median 672 µs on Forte's 30-ion chain).

Brief →

Key references

[100] J.-S. Chen et al., “Benchmarking a trapped-ion quantum computer with 30 qubits,” Quantum, … · 2024
[121] S.-A. Guo et al., “A site-resolved two-dimensional quantum simulator with hundreds of trap… · 2024
[102] A. C. Hughes et al., “Trapped-ion two-qubit gates with >99.99% fidelity without ground-sta… · 2025
[109] E. Tham et al., “Breakeven demonstration of quantum low-density parity-check codes,” arXiv… · 2026
[101] IonQ, “IonQ Tempo: 100-Qubit Quantum Computer (#AQ 64).” [Online]. Available: https://ionq…

Design space — attributes

(a) carrier affinity
natural
(b) time · entangling
—
(c) readout
—
(d) mobility
shared bus (motional / cavity)
(e) control
—
(f) error structure
coherent / calibration
(g) manufacturing
MEMS / surface-electrode traps

Evaluation space — dated attributes

independently benchmarked chain (Forte) → 30 ions, all 435 pairs
defines: count with quality · 2023-08 · source
largest chain demonstrated (Tempo development system) → 64-qubit register, #AQ 64 [C] — IonQ's own benchmark, no per-pair data; the 100-qubit product is listed for late 2026
defines: count with quality · 2025-09 · source

IonQ Forte is a 30-ion chain (435 pairs), not 36; the 100-ion all-to-all Tempo chain is a company claim with no published gate time or per-pair fidelity.

Standard records

connectivity degree → 29 · typical
IonQ Forte: 'single-chain 30-qubit trapped-ion quantum computer with all-to-all operations', benchmarked over all 30-choose-2 = 435 pairs · 2023-08 · source [D] ⓘ
transport per round → not published · typical
Not applicable: a single motional-bus chain performs no transport between zones; all 435 Forte pairs are addressed in place · 2023-08 · source [D] ⓘ

Edges

needs: Trapped atomic ion
needed by: Non-local qLDPC codes (bivariate bicycle, 'gross')°, High-rate concatenated codes with transversal gates°, Colour code (transversal Cliffords)°
alternatives: Ion shuttling (QCCD, junctions, grid traps)
conflicts with:
Mølmer–Sørensen / light-shift laser gate open — no mitigation shown at scale
gate time grows with chain length (median 672 µs on Forte's 30-ion chain)
price spectral crowding of the motional modes makes the gate slower and less faithful as the chain grows: median 672 µs on Forte's 30-ion chain vs ~10–30 µs on short chains
mitigation short chains in zoned QCCD traps (Quantinuum), amplitude/phase-modulated gates, or electronic gates on ≤ 4-ion segments · 2025
° one of several that would do · the usual route, not a strict need

Used by 18 machines (18 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 — Fig. 1: Quantum dynamics of an EASE gate.a An energy-level diagram associated with the pth motional mode showing off-resonant red and blue sideband…
Three-panel principle diagram: (a) energy levels of two ion qubits with a motional ladder, showing the red- and blue-sideband paths that couple |00⟩ to |11⟩; (b) the spectrum of the chain's motional modes on both sides of the qubit carrier, with the symmetric detuning μ of the gate pulses; (c) arrows giving how strongly each of 13 ions takes part in two chosen modes. It is Figure 1 of a 2020 Nature Communications article by Grzesiak, Blümel, Wright and co-authors on efficient arbitrary simultaneously entangling (EASE) gates on a trapped-ion quantum computer. It shows how shared motional modes let any ions of a chain be entangled. “Fig. 1 — Fig. 1: Quantum dynamics of an EASE gate.a An energy-level diagram associated with the pth motional mode showing off-resonant red and blue sideband transitions…” by Grzesiak et al., www.nature.com/articles/s41467-020-16790-9, CC BY 4.0 (creativecommons.org/licenses/by/4.0/)
File:Diagram of the Cirac-Zoller CNOT gate.svg
Black-and-white principle diagram: a chain of ions with two marked qubits, A and B, sharing a vibrational (phonon) mode, plus zoomed level schemes of each ion's ground, excited and auxiliary states with numbered laser pulses. Drawn by QuarksAndElectrons (2024-01-21) to illustrate the Cirac–Zoller gate: a π-pulse on ion A, a 2π-pulse on ion B, then another π-pulse on ion A. It shows how trapped-ion qubits interact through shared motion: the chain's vibration acts as a bus carrying ion A's state to ion B. “Diagram of the Cirac-Zoller CNOT gate” — QuarksAndElectrons, CC0 1.0. Source: commons.wikimedia.org/wiki/File:Diagram_of_the_Cirac-Zoller_…
Fig. 3 — Figure 3: (a) Illustration of a line of ions illuminated by two semi-global beams. (b) The corresponding coupling matrix Φ is split to B=2B=2 global…
A two-panel drawing: on the left a line of ten trapped ions lit by two wide laser beams, one covering each half; on the right a block matrix of the couplings between ions, within each beam and across the two. It comes from arXiv paper 2509.14331 by Yakov Solomons and co-authors. It shows how ions in one chain can all be coupled to each other through their shared motion, even with only a few broad beams; notice the mixed-colour block for couplings between the two halves. “Fig. 3 — Figure 3: (a) Illustration of a line of ions illuminated by two semi-global beams. (b) The corresponding coupling matrix Φ is split to B=2B=2 global…” by Yakov Solomons, Yotam Kadish, Lee Peleg, Jonathan Nemirovsky, Amit Ben Kish, Yotam Shapira, arxiv.org/abs/2509.14331, CC BY 4.0 (creativecommons.org/licenses/by/4.0/)
cx_bus · layer 4 Connectivity / transport · centrality 4.2 · demonstrated · since 2003 · updated 2026-09-30

Ion-chain motional bus (all-to-all in chain)

A shared collective motional mode entangles any pair in one trap, giving genuine all-to-all connectivity at the price of gate time growing with chain length.

Verdict. Real all-to-all to ~30 benchmarked ions and ~100 claimed; IonQ's 10,000-ions-on-one-chip target for 2027 has no published heating, gate-time or mode-spectrum data behind it.

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

Ions in one trap share collective motional modes; a spin-dependent force through a shared mode entangles any pair without moving them, so connectivity is all-to-all by construction. Cirac–Zoller (1995) and Mølmer–Sørensen (1999) gave the mechanism; chain gates date from 2003.
Bus mobility, one shared mode, no transport; MEMS-adjacent trap fabrication.
No control modality or readout of its own; coherent error — mode addressing and heating, not loss.

Physics & limits

N ions carry N motional modes in a fixed bandwidth, so mode spacing falls as ~1/N: a gate must resolve one mode spectrally, costing time, or close all with shaped pulses, costing power and calibration. Gate time therefore rises with chain length — 550–883 µs, median 672 µs, on a 30-ion chain against 110 µs for one qubit D[100]. Electrode noise heats the shared mode, and error grows with N as every pair borrows the same excitation. Above a critical anisotropy the chain buckles into a zigzag: long chains need weak axial confinement, hence lower frequencies and slower gates. The floor moves with laser-free electronic gates (2Q 8.4×10⁻⁵ D[102]) and shaped pulses.

Engineering state of the art

table
Date Figure Who Tag+key
2023-08 30-ion chain, 435 pairs benchmarked; MS 550–883 µs IonQ Forte D[100]
2024 512-ion 2D crystal, analogue only Tsinghua D[121]
2025-10 2Q error 8.4×10⁻⁵, electronic gate, no cooling IonQ/Oxford Ionics D[102]
2026-06 qLDPC memory break-even within error bars, 3.95±0.68 s (one code) vs 3.84±0.48 s physical (revised Sep 2026) IonQ D[109]

Tempo: 100 ions, #AQ 64, no gate time C[101]. Dominant term: gate time, not fidelity.

The chain's motional modes can also serve as a bosonic register rather than only as a gate bus. A three-ion ¹⁷¹Yb⁺ chain encoded a scalar field in one set of transverse modes (2.80–3.05 MHz) and evolved it with spin–phonon gates, avoiding the truncation of bosons into qubits, while Mølmer–Sørensen gates used the other transverse set so that the two do not interfere; measured phonon occupations matched simulation up to eight quanta per mode, and a fourth bosonic mode had to run in a separate circuit D[884]. The register is short-lived: motional coherence is ≲ 10 ms against ≈ 1.5 s of idle spin coherence D[884].

The 100-ion Tempo chain is a company claim; the largest independently benchmarked chain is 30 ions. Not published: Tempo's two-qubit gate time and per-pair fidelity, beyond #AQ 64 and a "99.9% fidelity" headline; KISTI's Tempo-100 contract value; and any heating, mode-spectrum or interconnect data that reconciles IonQ's 10,000-ions-on-one-chip 2027 target with the chain-length trade-off.

Manufacturing, materials & supply chain

IonQ closed its SkyWater acquisition on 2026-07-31, naming microfabricated-trap fabs in Minnesota, Florida and Texas, no wafer size or node disclosed Cfact. Control splits two ways: laser MS gates need several wavelengths and per-ion optics; electronic gates use on-chip current and microwave lines. At 10³ ions the wall is the mode spectrum, not wiring: the answer is many short chains joined by shuttling or photonics — IonQ's first two-system entanglement (2026-04-14) disclosed no rate or fidelity Cfact. Export exposure sits with the finished machine: ECCN 4A906 controls it only when its qubit count and C-NOT error fall in the same band, from 34–99 qubits at ≤ 10⁻⁴ to any error from 2,000 qubits fact; no rule names ion traps G[301].

Role in the stack

It is the primary connectivity of two trapped-ion architectures: the linear Paul trap with individual laser addressing and electronic qubit control (laser-free, microwave-driven gates). Requires nothing; provides the non-local checks bivariate bicycle qLDPC and high-rate transversal codes assume, as IonQ's eight codes on one 40-ion chain show, run without hardware reconfiguration, one of them at break-even within error bars D[109]. It competes with QCCD shuttling, which buys chain length with transport time: Helios gets all-to-all from a ring plus junction at ~55 ms per full-width layer D[97], and on H2 transport took ~60% of circuit time on average D[110]. Derived clock = sum of the syndrome round: gate layers + transport + readout + reset ≈ 1.5×10⁻³ s, gate layers 1.4 ms of it. Verification: Forte's figure is an all-pairs benchmark over 435 pairs, so position effects are visible; Tempo publishes #AQ 64 and "99.9% fidelity" with no gate time or per-pair data — a disclosure gap, not a dispute.

Actors & economics

Who.
| Organisation | Role | Country | What they do | Evidence |
|---|---|---|---|---|
| IonQ | developer | US | Forte and Tempo chains; owns SkyWater | C[101] |
| Oxford Ionics | developer | UK | Electronic laser-free gates; IonQ unit | D[102] |
| Quantinuum | developer | US/UK | Rival transport architecture | D[97] |
| eleQtron | developer | Germany | MAGIC microwave ion control | C[129] |

Money. 2025-09-17 · IonQ · M&A, Oxford Ionics · $1.075 B USD · closed fact. 2025-10-12 · IonQ · equity · $2.0 B USD at $93/share · closed fact. 2025-11-06 · DARPA · QBI Stage B · up to $15 M each · IonQ and Quantinuum among eleven G[65]. 2026-05-05 · eleQtron · Series A · €57 M · closed C[129]. 2026-07-31 · IonQ · M&A, SkyWater · ~$1.8 B USD · closed fact. 2026-08 · IonQ · Q2-2026 revenue $80.1 M (+287% YoY), cash $3.0 B C[326].

Market & supply chain. The bus buys a trap chip, lasers or microwave lines and one vacuum system; concentration risk sits with narrowband laser and AOM vendors, whom electronic gates remove. It pays into G3 and G5.

IP & standards. PatSnap names IonQ the filing leader on motional-mode engineering Pfact; no standards body.

Roadmaps & track record. (2025-06 · for 2026 · 256 qubits at 99.99% · slipped to H1 2027); (for 2027 · 10,000 on one chip · no heating data); (for 2030 · 2 M physical) R[132]. Fidelity claims land, scale dates do not: the 2020 roadmap promised 4,000 qubits by 2026, missed ~40×.

Strategic reading. If chain all-to-all holds to a few hundred ions, ion vendors keep the connectivity advantage that makes high-rate codes cheap, and IonQ's owned fabs speed trap iteration. If not, the bus is a module-internal detail and value moves to interconnects.

Outlook & open questions

Confirm if IonQ publishes Tempo gate times and per-pair fidelities, or ships 256 qubits in H1 2027; demote if disclosure stays headline-only. Best case 2029: electronic gates on owned-fab traps carry chains past 100 ions. Worst case: chains stall near 30–50 ions. Open: how does mode heating scale at 100 ions?

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. [97] A. Ransford et al., “A 98-qubit trapped-ion quantum computer with all-to-all connectivity,” Nature, vol. 655, no. 8121, pp. 81–86, Jun. 2026, doi: 10.1038/s41586-026-10676-4. arXiv:2511.05465. D
  3. [100] J.-S. Chen et al., “Benchmarking a trapped-ion quantum computer with 30 qubits,” Quantum, vol. 8, Art. no. 1516, Nov. 2024, doi: 10.22331/q-2024-11-07-1516. arXiv:2308.05071. D
  4. [101] IonQ, “IonQ Tempo: 100-Qubit Quantum Computer (#AQ 64).” [Online]. Available: https://ionq.com/quantum-systems/tempo C
  5. [102] A. C. Hughes et al., “Trapped-ion two-qubit gates with >99.99% fidelity without ground-state cooling,” arXiv:2510.17286, Oct. 2025. D
  6. [109] E. Tham et al., “Breakeven demonstration of quantum low-density parity-check codes,” arXiv:2606.06455, Jun. 2026. D
  7. [110] S. A. Moses et al., “A Race Track Trapped-Ion Quantum Processor,” Phys. Rev. X, vol. 13, Art. no. 041052, Dec. 2023, doi: 10.1103/PhysRevX.13.041052. arXiv:2305.03828. D
  8. [121] S.-A. Guo et al., “A site-resolved two-dimensional quantum simulator with hundreds of trapped ions,” Nature, vol. 630, no. 8017, pp. 613–618, May 2024, doi: 10.1038/s41586-024-07459-0. D
  9. [129] A. Cordes, “Quantum computing scale-up eleQtron secures €57 million in one of the largest Series A funding rounds worldwide,” eleQtron, May 5, 2026. [Online]. Available: https://eleqtron.com/en/quantum-computing-scale-up-eleqtron-secures-57-million-in-one-of-the-largest-series-a-funding-rounds-worldwide/ C
  10. [132] IonQ, “IonQ's Accelerated Roadmap: Turning Quantum Ambition into Reality,” Jun. 13, 2025. [Online]. Available: https://www.ionq.com/blog/ionqs-accelerated-roadmap-turning-quantum-ambition-into-reality R
  11. [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
  12. [326] IonQ, “IonQ Announces Record Second Quarter 2026 Revenues, Growing 287% YoY,” Aug. 5, 2026. [Online]. Available: https://www.ionq.com/news/ionq-announces-record-second-quarter-2026-revenues-growing-287-yoy C
  13. [884] A. T. Than et al., “Quantum field theory dynamics on a spin–phonon quantum computer,” Nat. Phys., Sep. 2026, doi: 10.1038/s41567-026-03402-4. arXiv:2509.11477. D