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Multi-chip modules / l-couplers (same cryostat) ic_mcm

Splitting a superconducting processor across several dies inside one cryostat, joined by bump-bonded chiplet links or metre-scale superconducting l-couplers.

Multi-chip modules / l-couplers (same cryostat)

ic_mcm · layer 9 Interconnect · emerging · since 2025

Chiplet tiling (Rigetti 12×9 q, 99.1%) and metre-scale l-couplers between modules (IBM Cockatoo 2027 [R]).

Reading marks
crossing technology — fabricated carrier + far connectivity (transport / long-range)
Brief →

Key references

[747] A. Gold et al., “Entanglement across separate silicon dies in a modular superconducting qu… · 2021
[748] J. Niu et al., “Low-loss interconnects for modular superconducting quantum processors,” Na… · 2023
[481] R. Mandelbaum et al., “How IBM will build the world's first large-scale, fault-tolerant qu… · 2025
[750] Y. Martin et al., “Mechanically-intermixed indium superconducting connections for microwav… · 2024
[749] M. Field et al., “Modular Superconducting Qubit Architecture with a Multi-chip Tunable Cou… · 2023

Design space — attributes

(a) carrier affinity
fabricated
(b) time · entangling
—
(c) readout
—
(d) mobility
long-range static couplers
(e) control
microwave @ millikelvin stage
(f) error structure
coherent / calibration
(g) manufacturing
superconducting lithography

Evaluation space — dated attributes

chiplet tiling → 108 q from 12 chiplets, median 2Q 99.1% (vs 99.5% at 36 q)
defines: count with quality · 2026-04 · source
coupled cryogenic cells → two cells coupled; 0.53 m² wiring area each
defines: scaling path · 2026-08 · source

Used by 13 machines (12 primary · 1 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. 5 — Figure 5: Resistance measurements before and after replacing modules. (a) The normalized resistance vs. temperature. The measurement starts at the b…
A small four-panel paper figure. (a) Normalized resistance versus temperature (3–8 K) of two chip-to-chip interconnects, “Chip 1 and 2” and “Chip 1 and 4”, each falling to zero in two steps, near 6 K and at 4.3–4.7 K; (b)–(d) tiny optical micrographs of a liquid-metal strip bridging the seam between two chips: before, after a chip swap (a bare gold pad shows), and reconnected. It is Fig. 5 of arXiv 2603.09096 (March 2026) by Zhancheng Yao, … David J. Bishop, on reconfigurable superconducting quantum circuits with micro-scale liquid-metal interconnects. Notice the joint still becomes superconducting after the chip is replaced; the chips are test chips, not qubit processors. “Fig. 5 — Figure 5: Resistance measurements before and after replacing modules. (a) The normalized resistance vs. temperature. The measurement starts at the base…” by Zhancheng Yao, Nicholas E. Fuhr, Nicholas Russo, David W. Abraham, Kevin E. Smith, David J. Bishop, arxiv.org/abs/2603.09096, CC BY 4.0 (creativecommons.org/licenses/by/4.0/)
Fig. 3 — Figure 3: Physical qubit layouts at the interface and the corresponding gate sequences for inter-chip syndrome extraction. Blue (red) plaquettes den…
A two-part drawn schematic, not a photograph: (a) a rotated surface-code patch of red and blue stabilizer plaquettes split by a dashed chip-to-chip seam, with buffer qubits as squares and inter-chip gates in green; (b) the gate sequence for one X-stabilizer straddling the seam. It is Figure 3 of "Taming Spacetime Overhead and Design Complexity in Distributed Fault-Tolerant Superconducting Quantum Computation" by Qinjing Yu and Ke Liu. It shows how buffer qubits let slower inter-chip links run one surface code across chips; note the long green inter-chip window. “Fig. 3 — Figure 3: Physical qubit layouts at the interface and the corresponding gate sequences for inter-chip syndrome extraction. Blue (red) plaquettes denote…” by Qinjing Yu, Ke Liu, arxiv.org/abs/2608.23159, CC BY 4.0 (creativecommons.org/licenses/by/4.0/)
Fig. 3 — Figure 3: cQAD device based on a microring cavity. a, Schematic of the flip-chip assembly. The phononic microring cavity is fabricated on a top chip…
A seven-panel paper figure: a 3D render of two stacked chips (11 mm and 15 mm square), optical micrographs of a phononic ring resonator and of the qubit chip, and data plots. It comes from the arXiv paper "Circuit Quantum Acoustodynamics in a Scalable Phononic Integrated Circuit Architecture" by Weiting Wang, Luyan Sun and co-authors. It shows a superconducting transmon qubit on one chip talking to a sound resonator on another: an interdigital transducer on the ring and facing capacitor pads link the two across the flip-chip gap. “Fig. 3 — Figure 3: cQAD device based on a microring cavity. a, Schematic of the flip-chip assembly. The phononic microring cavity is fabricated on a top chip of 11 mm…” by Weiting Wang et al., arxiv.org/abs/2512.04953, CC BY 4.0 (creativecommons.org/licenses/by/4.0/)
ic_mcm · layer 9 Interconnect · centrality 13.9 · emerging · since 2025 · updated 2026-09-30

Multi-chip modules / l-couplers (same cryostat)

Splitting a superconducting processor across several dies inside one cryostat, joined by bump-bonded chiplet links or metre-scale superconducting l-couplers.

Verdict. Chiplet tiling ships and costs fidelity — 99.5% at four chiplets, 99.1% at twelve; l-couplers have no published fidelity. Demote if no two-module entangling figure by end-2027.

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 multi-chip module partitions one processor across several superconducting dies sharing a single dilution refrigerator, with quantum-coherent links between them. Two different links wear the label. The short one is a chiplet join: dies flip-chip mounted on a common carrier at sub-millimetre pitch, coupled through indium bumps or vacuum-gap capacitors, so an inter-die coupler is electrically a slightly longer on-chip coupler. The long one is IBM's "l-coupler", a superconducting cable of centimetre-to-metre length carrying a microwave mode between separately packaged modules under one mixing chamber. Both differ from inter-fridge links, which cross a room-temperature gap, and from on-chip long-range couplers, which never leave the die.

Lineage: Rigetti entangled qubits across four separate silicon dies in 2021-09, iSWAP 99.1 ± 0.5% and CZ 98.3 ± 0.3%, with a Bell violation between dies D[747]; SUSTech linked five modules with aluminium coaxial interconnects in 2023-02 D[748]; IBM says l-couplers were "first demonstrated in 2024" on Flamingo C[481], and in 2024-09 published low-loss indium joins for the superconducting cables of such links, tested on 1 m of aluminium coax with no qubit measured through it D[750]. The graph record dates the node to 2025, when tiling became a shipped product rather than a demonstration.

Attributes. Affinity: fully fabricated, a packaging structure with no natural counterpart. Characteristic time and determinism: not applicable — the node carries no entangling primitive, it inherits the gate it transports. Readout: none. Mobility: long-range, the property it exists to supply. Control: microwave at millikelvin. Error structure as the code sees it: coherent. Manufacturing: superconducting lithography plus packaging steps.

Physics & limits

The short-link floor is frequency crowding, not loss. Each chiplet is a separate fabrication instance with its own junction-resistance distribution, so tiling k dies convolves k frequency distributions that were never co-targeted; collisions between qubit, coupler and inter-die modes are fixed at packaging time and cannot be tuned away. Hence the coherent error structure: a mis-set detuning is a deterministic phase, not a stochastic click. The bonds themselves are benign — Rigetti's multi-chip tunable couplers, built from vacuum-gap capacitors or indium bumps, reached a CZ of 99.13 ± 0.15% in 56 ns through a coupler bridging four chips, "at the same level" as a single-chip tunable coupler, with no coherence penalty from one or more bonds D[749].

The long-link floor is cable loss and mode density. A metre-scale cable is a multimode resonator whose free spectral range is of order 100 MHz, so tens of modes fall in the 3–5.5 GHz band the qubits use D[750]. Loss sets transfer error: at an internal quality factor of 1.24 × 10⁶ on an indium press-mold cable-to-chip join, photon lifetime is Q/ω ≈ 49 µs, so a 100 ns inter-module SWAP costs about 2 × 10⁻³ S[750]. Joins dominate in practice — contact resistances of 6 × 10⁻⁴ Ω at an inner-conductor splice and 8.5 × 10⁻⁴ Ω cable-to-chip are the measured levers D[750].

Underneath both is a yield argument: monolithic yield falls as y^N in qubit count, and tiling k chiplets of n qubits replaces one exponential with k smaller ones plus an assembly step. The price shows in the only shipped data, 99.5% at four chiplets against 99.1% at twelve C[36], [751]. Moving the floor needs co-targeted junction trimming across a chiplet set Dfact and joins whose loss and mode comb stay out of the way.

Engineering state of the art

Best demonstrated as of 2026-09-03: inter-module SWAP at the 99% level in under 100 ns between two modules in one cryostat, remote-entanglement error near 1% D[752]. Typical at scale: Rigetti's Cepheus-1-108Q, 108 qubits from twelve 9-qubit chiplets, median two-qubit 99.1%, single-qubit 99.9%, ~60 ns gates C[36]. No l-coupled processor exists; IBM's 2026 milestone is two coupled cryogenic cells with no qubits in them C[50].

Records timeline
Year Figure Who Tag+key
2021-09 iSWAP 99.1 ± 0.5%, CZ 98.3 ± 0.3% across four dies; Bell violation Rigetti D[747]
2023-02 five modules on Al coax, Q 8.1 × 10⁵, transfer and Bell 99%, 12-qubit GHZ 55.8 ± 1.8% SUSTech D[748]
2023-08 CZ 99.13 ± 0.15% in 56 ns through a coupler bridging four chips Rigetti D[749]
2024-09 indium cable-to-chip join, Q 1.24 × 10⁶, contact resistance 8.5 × 10⁻⁴ Ω IBM D[750]
2025-06 inter-module SWAP 99% in < 100 ns, remote entanglement error ≈ 1% Illinois D[752]
2025-07-16 36 qubits, four chiplets, median 2Q 99.5%, 2× error cut vs Ankaa-3 Rigetti C[751]
2026-04-07 108 qubits, twelve chiplets, median 2Q 99.1% Rigetti C[36]
2026-08-19 two cryogenic cells coupled; 0.53 m² wiring, 2.75 m³ vacuum per cell IBM C[50]

The dominant term is not the interconnect. Rigetti's own comparison isolates it: same chiplet, same join, three times as many, 40 basis points of two-qubit fidelity lost C[36], [751]. Nothing published attributes that loss, which makes frequency targeting across a tiled set the leading suspect and the leading unknown.

Manufacturing, materials & supply chain

Superconducting lithography plus a packaging line: flip-chip bonding, indium bumps or press-mold joins, through-silicon vias, a carrier. IBM builds on 300 mm at Albany NanoTech Cfact; QuantWare sells 3D vertical integration as a product — a stack of chiplet modules with chip-to-chip connections targeting 10,000 qubits, first delivery 2028, with a Kilofab in Delft opening 2026 to raise capacity 20× P[495]fact. Rigetti fabricates 9-qubit chiplets on its own line C[751].

The single points of failure sit outside the fab. The cryostat is one: IBM's cell architecture is a bespoke refrigerator programme, and the merchant alternative is Bluefors' KIDE, quoted at more than 4,000 RF lines and "over 1000 qubits" on nine pulse tubes Cfact. Bump-bond and TSV capacity for superconducting stacks sits with a handful of lines — Albany, Kilofab, GlobalFoundries under its CHIPS letter of intent fact, SkyWater now inside IonQ fact. Export exposure is uneven. The BIS rule of 2024-09-06 puts dilution refrigerators rated ≥ 600 µW at ≤ 0.1 K under ECCN 3A904, but a quantum computer under 4A906 only when its qubit count and its C-NOT (controlled-NOT gate) error fall in the same band — 34–99 qubits at ≤ 10⁻⁴, 100–199 at ≤ 10⁻³, the ceiling rising to 6 × 10⁻³ below 2,000 qubits, any error from 2,000 on fact. Rigetti's 108 qubits at a median two-qubit error near 9 × 10⁻³ C[36] fall outside 4A906, so a refrigerator of that class can be controlled while the tiled processor it cools is not.

Control, readout & I/O burden

Packaging does not reduce lines per qubit; it relocates them and buys wiring area. At 10³ qubits one merchant cryostat suffices — KIDE's 4,000-plus RF lines cover it Cfact. At 10⁴ the choice is 40,000 lines through vertical I/O, QuantWare's 2028 promise Pfact, or cold multiplexing. At 10⁶ neither works: many cells plus on-chip control generation, whose published pointer is millikelvin SFQ control at 1Q > 99% fact.

Latency is not the l-coupler's problem — the demonstrated inter-module SWAP is under 100 ns D[752] against a 280 ns readout at 99.94% fidelity D[38]. The decoder is: cross-module syndrome extraction must close inside a ~1 µs cycle while a parity check spans two packages, and no such demonstration exists as of 2026-09-03. NVQLink's 3.84 µs round trip Pfact is a host-QPU budget, far too slow for an intra-cryostat check.

Role in the stack

Three architectures use it: superconducting transmons, superconducting bosonic cat/GKP, superconducting dual-rail erasure. It requires superconducting-qubit lithography with multilayer routing and flip-chip packaging. It replaces inter-fridge cryogenic links, and the price is thermal: everything shares one cooling budget and one vacuum, so scaling stops at the fridge rather than at the network. Its contribution is manufacturability, not gate physics.

A fabricated carrier acquires far-range connectivity through packaging, where atoms and ions acquire it through motion. Derived clock = sum of the syndrome round: gate layers + transport + readout + reset for the architecture: 0.65 µs, readout at ≈ 280 ns its largest term, and the < 100 ns inter-module SWAP D[752] is at most about 15% of the round (100 of 650 ns), so transport does not bind. Neighbouring empty slots: cross-module error correction, and a qLDPC code whose checks span modules — compilation for such machines exists only in simulation S[753].

Evidence — how the numbers were measured

Rigetti's 99.1% and 99.5% are company medians without error bars or a stated protocol C[36], [751]; the 2021 die-to-die numbers carry explicit uncertainties D[747]. SUSTech's 99% is a state-transfer and Bell-state fidelity, not a gate fidelity, and its 12-qubit GHZ at 55.8 ± 1.8% shows what five linked modules do at depth D[748]. The Illinois figure is a SWAP efficiency with a separately stated ~1% error called threshold-level; the two should not be conflated D[752]. IBM's coupled-cell result contains no qubits and no fidelity claim C[50]. No value conflicts were found; the gap is that nothing explains the 99.5% → 99.1% step.

Neither arXiv:2308.09240 (Rigetti; cross-chip CZ 99.13 ± 0.15% in 56 ns) nor arXiv:2409.04634 (IBM Quantum, T. J. Watson Research Center; cable joins, no qubit measured) has a journal version as of 2026-09-30. The 40,000 I/O lines of QuantWare's Bass-A10K (VIO-40K) rest only on QuantWare's own release of 2025-12-08 fact, which the trade-press page of 2025-12-10 P[495] omits, and no delivered device confirms them. Not published: a gate fidelity or latency through IBM's l-coupler, "first demonstrated in 2024" on Flamingo C[50], [481], whose cable joins were tested on 1 m of aluminium coax at internal Q ≈ 10⁶ D[750], as of 2026-09-30; and a dated assignee record for Rigetti's chiplet-packaging and QuantWare's vertical-I/O patent families.

Actors & economics

Who.
Organisation Role Country What exactly they do with this technology Evidence
IBM developer US l-couplers between modules and their cable joins; modular cryogenic cells; Cockatoo 2027, Starling 2029 C[50], [481] D[750] fact
Rigetti developer US only shipped multi-chip system with published figures: 4- and 12-chiplet processors C[36], [751] fact
QuantWare supplier Netherlands merchant 3D-integrated chiplet stacks; VIO-40K, Kilofab Delft P[495] fact
SUSTech research CN five-module aluminium-coax interconnect network D[748]
Univ. of Illinois Urbana-Champaign research US interchangeable modules, 99% inter-module SWAP < 100 ns D[752]
Bluefors supplier FI KIDE platform, > 4,000 RF lines, the merchant multi-module fridge Cfact
GlobalFoundries supplier US multi-modality foundry under CHIPS letter of intent, $375 M fact
DARPA funder US QBI Stage B funds IBM's modular path; Rigetti not on the list fact

Money.

  • 2025-11-06 · IBM · DARPA QBI Stage B selection · up to $15 M each · DARPA · announced fact
  • 2026-05-05 · QuantWare · Series B · $178 M (€152 M) · Intel Capital, In-Q-Tel, ETF Partners, no single lead · cumulative > $210 M · closed Pfact
  • 2026-05-21 · Rigetti · CHIPS letter of intent · up to $100 M · Dept of Commerce, within a $2.013 B package (GlobalFoundries $375 M, IBM/Anderon $1 B) · LOI, non-binding fact
  • 2026-07-31 · IonQ · acquisition of SkyWater Technology · ~$1.8 B at announcement · closed fact
  • 2026-08 · Rigetti · Q2-2026 results · revenue $5.1 M, GAAP loss $52.6 M, cash $541.3 M · reported fact

Market & supply chain. No one sells an l-coupler; it is a captive design block. The merchant layer is one company deep — QuantWare is the only vendor selling 3D-integrated multi-chip QPUs to third parties P[495] — plus Bluefors for the enclosure and a short list of lines that can do superconducting flip-chip at volume. Who pays: G3 and G4 above all, since Starling depends on modules rather than a bigger die; G7 for deployable multi-cell systems; G2 through wider processors.

IP & standards. IBM holds US 12,517,856, "Modular quantum system with discrete levels of connectivity" (filed 2022-09-28, granted 2026-01-06), and US 12,587,192 on chains of resonators with tunable inductive couplers (granted 2026-03-24) fact — the l-coupler's cable joins are published D[750], a gate fidelity through one is not. For Rigetti's chiplet packaging and QuantWare's vertical I/O, no dated patent fact was found within budget. There is no inter-module interface standard and no open-source packaging stack.

Roadmaps & track record.

  • IBM: promised 2025-06-10 · l-couplers demonstrated on Flamingo in 2024 · claimed delivered, no link fidelity published as of 2026-09-30 C[481].
  • IBM: promised 2025-06-10 · Cockatoo 2027, entanglement between modules via the universal adapter; Nighthawk on nine l-coupled modules for 1,080 qubits by 2028 · pending R[481] fact.
  • IBM: promised 2022-05-10 · Kookaburra, a 1,386-qubit multi-chip processor, for 2025 C[313]; re-promised 2025-06-10 for 2026 as the first module with a qLDPC memory R[481] · not delivered as of 2026-09-30 fact.
  • Rigetti: promised 2025-07-16 · 100+ qubit chiplet system at median 99.5% before end-2025 · delivered 2026-04-07 at 99.1%, target moved to "later in 2026" C[36], [751].
  • QuantWare: promised 2025-12-08 · VIO-40K (VIO is QuantWare's vertical-wiring architecture), 10,000 qubits, first delivery 2028 · pending Pfact.

Credibility: IBM meets its single-chip processor dates but not its multi-chip one — Kookaburra, promised for 2025, is undelivered — and publishes packaging as architecture rather than measurement, so its modular claims stay unfalsifiable until Cockatoo; Rigetti ships what it describes, a fidelity step behind its own target; QuantWare has money and a fab but no delivered multi-chip QPU at scale to judge.

Strategic reading. If multi-chip modules work, the decisive asset moves from lithography to packaging and cryogenics, and the winner is whoever controls bump-bond, TSV and fridge capacity — IBM by vertical integration, QuantWare by merchant supply, IonQ through SkyWater. The loser is any roadmap assuming a single ever-larger die. Substitution threats: on-chip long-range couplers, which buy connectivity without packaging risk, and inter-fridge links, which buy unlimited scale at the price of a room-temperature crossing. Supplier bargaining power is high: there are more credible qubit vendors than lines that can bond them.

Outlook & open questions

Confirm within 12–24 months if: IBM's Cockatoo demonstrates entanglement between two l-coupled modules with a published fidelity by end-2027 R[481]; Rigetti's 108-qubit system reaches median 99.5% C[36]; anyone runs a stabiliser round whose checks cross a module boundary. Demote if no l-coupler fidelity is published by end-2027. Best case by 2029: a few thousand qubits in coupled cells with cross-module error correction at Λ comparable to monolithic. Worst case: tiling saturates near 10² qubits because frequency targeting across dies does not scale.

Open questions: what causes the 40-basis-point tiling tax, per-join or per-calibration? Can a metre-scale cable's mode comb be pushed out of band without shortening it? What is an l-coupler's fidelity, two years after the claim? Does a qLDPC check spanning modules survive the extra transport error? Watch Rigetti's roadmap update, IBM's first Cockatoo measurement, QuantWare's Kilofab yield, and any paper benchmarking a chiplet boundary as such.

References
  1. [36] Rigetti Computing, Inc., “Rigetti Announces General Availability of 108-Qubit System,” Apr. 7, 2026. [Online]. Available: https://investors.rigetti.com/news-releases/news-release-details/rigetti-announces-general-availability-108-qubit-system C
  2. [38] F. Marxer et al., “Above 99.9% Fidelity Single-Qubit Gates, Two-Qubit Gates, and Readout in a Single Superconducting Quantum Device,” PRX Quantum, vol. 7, Art. no. 020333, 2026, doi: 10.1103/n86s-2b88. arXiv:2508.16437. D
  3. [50] C. Dundon, S. Hall, M. Hollister, and A. Lindler, “IBM's new modular architecture for cryogenic systems,” IBM Quantum Computing Blog, Aug. 19, 2026. [Online]. Available: https://www.ibm.com/quantum/blog/modular-cryogenics C
  4. [313] J. Gambetta, “Expanding the IBM Quantum roadmap to anticipate the future of quantum-centric supercomputing,” IBM Quantum Blog, May 10, 2022. [Online]. Available: https://www.ibm.com/quantum/blog/ibm-quantum-roadmap-2025 C
  5. [481] R. Mandelbaum et al., “How IBM will build the world's first large-scale, fault-tolerant quantum computer,” IBM Quantum Computing Blog, Jun. 10, 2025. [Online]. Available: https://www.ibm.com/quantum/blog/large-scale-ftqc C
  6. [495] M. Abdel-Kareem, “QuantWare Debuts VIO-40K™ Architecture to Enable 10,000-Qubit Superconducting Processors,” Quantum Computing Report, Dec. 10, 2025. [Online]. Available: https://quantumcomputingreport.com/quantware-debuts-vio-40k-architecture-to-enable-10000-qubit-superconducting-processors/ P
  7. [747] A. Gold et al., “Entanglement across separate silicon dies in a modular superconducting qubit device,” npj Quantum Inf., vol. 7, no. 1, Art. no. 142, Sep. 2021, doi: 10.1038/s41534-021-00484-1. arXiv:2102.13293. Also https://arxiv.org/abs/2102.13293. D
  8. [748] J. Niu et al., “Low-loss interconnects for modular superconducting quantum processors,” Nat. Electron., vol. 6, no. 3, pp. 235–241, Feb. 2023, doi: 10.1038/s41928-023-00925-z. arXiv:2302.02751. D
  9. [749] M. Field et al., “Modular Superconducting Qubit Architecture with a Multi-chip Tunable Coupler,” arXiv:2308.09240, Aug. 2023. D
  10. [750] Y. Martin et al., “Mechanically-intermixed indium superconducting connections for microwave quantum interconnects,” arXiv:2409.04634, Sep. 2024. D
  11. [751] Rigetti Computing, “Rigetti Demonstrates Industry's Largest Multi-Chip Quantum Computer; Halves Two-Qubit Gate Error Rate,” Rigetti Investor Relations, Jul. 16, 2025. [Online]. Available: https://investors.rigetti.com/news-releases/news-release-details/rigetti-demonstrates-industrys-largest-multi-chip-quantum C
  12. [752] M. Mollenhauer, A. Irfan, X. Cao, S. Mandal, and W. Pfaff, “A high-efficiency elementary network of interchangeable superconducting qubit devices,” Nat. Electron., vol. 8, no. 7, pp. 610–619, Jul. 2025, doi: 10.1038/s41928-025-01404-3. D
  13. [753] Z. Du et al., “Hardware-aware Compilation for Chip-to-Chip Coupler-Connected Modular Quantum Systems,” arXiv:2505.09036, May 2025. S