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Cross-resonance (fixed-frequency, all-microwave) g_cr

All-microwave entangling gate driving one fixed-frequency transmon at its neighbour's frequency through a static bus; no flux line, no tunable coupler.

Cross-resonance (fixed-frequency, all-microwave)

g_cr · layer 3 Gate mechanism · demonstrated · since 2011

Microwave-only entangling gate on fixed-frequency transmons; 180–500 ns; superseded by tunable couplers in IBM Heron.

Brief →

Key references

[425] J. M. Chow et al., “Simple All-Microwave Entangling Gate for Fixed-Frequency Superconducti… · 2011
[287] A. Kandala et al., “Demonstration of a High-Fidelity CNOT Gate for Fixed-Frequency Transmo… · 2021
[426] C. Kim, J. Kang, and Y. Kwon, “Lattice patch structure for fixed-frequency transmon quantu… · 2026
[34] IBM Quantum, “What's new at IBM Quantum - Q2 2026.” [Online]. Available: https://www.ibm.c…
[72] IBM, “Quantum Roadmap.” [Online]. Available: https://www.ibm.com/roadmaps/quantum/

Design space — attributes

(a) carrier affinity
fabricated
(b) time · entangling
316 ns · deterministic
(c) readout
—
(d) mobility
static nearest-neighbour wiring
(e) control
microwave @ room temperature
(f) error structure
coherent / calibration, stochastic Pauli
(g) manufacturing
superconducting lithography

Evaluation space — dated attributes

CR CNOT with intrinsic static-ZZ suppression (Kandala) → 99.77(2)% in a single 180 ns pulse
defines: error channel · 2021 · source

Kandala 2021 suppresses the static ZZ intrinsically (two fixed coupling elements retuning the dressed levels), not by an active cancellation drive; the pulse is 180 ns, not 320 ns. CR stayed IBM's native gate through Condor; Heron introduced the tunable-coupler CZ.

Standard records

2Q error under full-width parallel operation → 0.017 · typical
ibm_sherbrooke (Eagle r3, 127 q, fixed-coupling CR): EPLG 1.7e-2 at chain length 100 (layer fidelity 0.19); 0.26 at N=80 · 2023-11 · source [D] ⓘ
crosstalk → not published · typical
No simultaneous-minus-isolated crosstalk figure is published for cross-resonance; Kandala 2021 reports static-ZZ suppression, not a rate · 2021-09 · source [D] ⓘ

Actors & goals — annotations

Transmon lattice with tunable couplers (alternate) — IBM (Heron, Nighthawk), Google (Willow), Rigetti, IQM, OQC, USTC/Zhejiang, Fujitsu/RIKEN, QuantWare · G2 G3 G4

Edges

needs: Transmon, Room-temperature electronics + per-qubit coax/flex°, Cryo-CMOS controller (4 K / mK)°
alternatives: Tunable-coupler CZ / iSWAP
conflicts with:
Rotated surface code (+ yoked variants) bypassed by choosing another technology in place of one of the two
collision-free fixed frequencies force a sparse heavy-hex lattice; the degree-4 surface code then needs flag qubits and longer rounds
price a cross-resonance lattice avoids frequency collisions by keeping the degree at 2–3 (heavy-hex); the surface code's weight-4 checks then need flag qubits, a longer syndrome circuit and a lower threshold than on a degree-4 lattice
mitigation tunable couplers (g_tc) — IBM's move from Eagle's cross-resonance to Heron's tunable couplers, still on heavy-hex; the degree-4 square lattice came with Nighthawk (2025); or heavy-hex codes on the cross-resonance lattice · 2020-01
° one of several that would do · the usual route, not a strict need

Used by 6 machines (6 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. 6 — Figure 6: Optimization for the cross-resonance gate Z​X​(π/2)ZX(/2). We display results with fidelity over 99.9% for the direct and RL approaches at…
Simulated plots in three columns: a two-qubit ZX(π/2) gate by a smooth flat-top 'direct' pulse at 248.9 ns and by reinforcement-learning pulses at 248.9 ns and 177.8 ns. Rows (a, b) show pulse amplitudes on the cross-resonance and target drives; (c, d) the target qubit's ⟨X⟩, ⟨Y⟩, ⟨Z⟩ over time for control in |0⟩ or |1⟩, with Bloch-sphere insets. It is Figure 6 of 'Reinforcement learning pulses for transmon qubit entangling gates' (arXiv 2311.03684) by Ho Nam Nguyen, Felix Motzoi and co-authors. The cross-resonance gate entangles fixed-frequency transmons; the learned pulses are stepped, yet the caption reports over 99.9% fidelity; the target ends at opposite ⟨Y⟩ per control state. “Fig. 6 — Figure 6: Optimization for the cross-resonance gate Z​X​(π/2)ZX(/2). We display results with fidelity over 99.9% for the direct and RL approaches at gate…” by Ho Nam Nguyen, Felix Motzoi, Mekena Metcalf, K. Birgitta Whaley, Marin Bukov, Markus Schmitt, arxiv.org/abs/2311.03684, CC BY 4.0 (creativecommons.org/licenses/by/4.0/)
File:Keynote - Entering the Era of Quantum Utility (IBM Research) 06.png
A frame from a keynote video: a slide titled 'Tunable Coupler architecture – Performance' with a small render of an IBM Quantum processor, a line drawing of a heavy-hex qubit layout, and text comparing Eagle R3 with Heron R1. It comes from IBM Research's keynote 'Entering the Era of Quantum Utility' (IBM Quantum Summit 2023). It contrasts fixed-frequency cross-resonance (ECR) gates with tunable-coupler CZ gates on superconducting processors: notice Heron's 96 ns CZ versus Eagle's 537 ns ECR, allowing more gates despite a shorter mean T1. “Keynote - Entering the Era of Quantum Utility (IBM Research) 06” by IBM Research, commons.wikimedia.org/wiki/File:Keynote_-_Entering_the_Era_o…, CC BY 3.0 (creativecommons.org/licenses/by/3.0/)
Fig. 3 — NL-based benchmarking using LR-QAOA for WMC problems; (a) QPU layouts used in each experiment
Three-panel paper figure made of drawings and data plots, from an arXiv paper by J. A. Montanez-Barrera, Kristel Michielsen and David E. Bernal Neira (2025-05-28) on benchmarking processors with linear-ramp QAOA. Panel (a) draws the qubit coupling graphs of 5-, 20-, 127-, 133- and 156-qubit processors, including IBM Heron devices; panels (b) and (c) plot approximation ratio against the number of QAOA layers. Notice the fixed nearest-neighbour lattices: the sparse heavy-hex patterns versus the denser square lattice limit which qubits can interact directly. “Fig. 3 — NL-based benchmarking using LR-QAOA for WMC problems; (a) QPU layouts used in each…” by J. A. Montanez-Barrera, Kristel Michielsen, David E. Bernal Neira, arxiv.org/abs/2502.06471, CC BY 4.0 (creativecommons.org/licenses/by/4.0/)
g_cr · layer 3 Gate mechanism · centrality 4.2 · demonstrated · since 2011 · updated 2026-09-04

Cross-resonance (fixed-frequency, all-microwave)

All-microwave entangling gate driving one fixed-frequency transmon at its neighbour's frequency through a static bus; no flux line, no tunable coupler.

Verdict. Superseded on IBM's own fleet at Heron (2023-12) yet still the only two-qubit gate needing zero coupler control; it returns only if post-fabrication frequency trimming beats a flux DAC per coupler on cost.

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

Driving a control transmon at its neighbour's frequency through a fixed bus produces a ZX interaction (Z on the control, X on the target); Chow, Córcoles, Gambetta et al. (IBM), 2011 D[425]. Kandala et al. reached CNOT 99.77(2)% in a single 180 ns pulse in 2021 by suppressing the static ZZ intrinsically, two fixed-frequency coupling elements retuning the dressed levels rather than extra cancellation drives D[287].
Attributes: fabricated carrier, static connectivity, microwave control at room temperature; deterministic entangling at 10^-6.5 s (~320 ns typical, 180 ns best).
Coherent plus Pauli error; standard superconducting lithography, no added process.

Physics & limits

The ZX rate is second order, ∝ JΩ/(Δ(Δ+α)), fastest in the straddling regime −α < Δ < 0, so the detuning must sit inside a band of order the anharmonicity, ~300 MHz. The static ZZ, ∝ 2J²α/(Δ(Δ+α)), never switches off, so coherent error dominates the budget. The floor is not one pair but frequency targeting: every neighbour adds a collision constraint inside that band, and junction spread as fabricated is of order a per cent, so collision-free yield collapses with lattice size. What moves the floor is post-fabrication trimming — annealing junctions to target, 97.4% success D[294] — not better pulses.

Engineering state of the art

table
Date Figure Who Tag
2011 First all-microwave CR entangling gate IBM D[425]
2021-09-22 CNOT 99.77(2)% in a single 180 ns pulse IBM D[287]
2026-06-25 Fixed-frequency lattice patch, CNOT > 98% simulated Hanyang University S[426]

No fleet-average cross-resonance (CR) number was ever published; IBM's EPLG today (3.7×10⁻³ D[34]) is Heron hardware, which replaced CR in 2023-12 C[72]. The painful reference is Oxford/OQC's fixed-coupling CZ, 99.8% in 25 ns C[423] — no coupler control either, seven times faster.

The PRL by Kandala et al. reports intrinsic ZZ suppression through two fixed-frequency coupling elements, not active cancellation. Not published: a fleet-average CR fidelity for IBM's pre-Heron generations (Falcon to Condor), beside the isolated-pair 99.77(2)%, and a dated CR-specific patent count.

Manufacturing, materials & supply chain

No process of its own. The cost lands in binning and trimming: a collision cannot be detuned away after fabrication, only masked in software or annealed out, so frequency targeting — laser annealing at IBM, alternating-bias annealing at Rigetti D[294] — is the supply-chain item CR drives. Its advantage is the I/O ledger: one drive line per qubit and nothing per coupler, where tunable couplers add a flux line and a DAC channel each, roughly 1.5–2× the lines. At 10³ that is a crowded fridge against an impossible one; at 10⁴–10⁶ it is the whole wiring budget. Export exposure is the carrier's (ECCN 3A901).

Role in the stack

The fixed-frequency branch of the transmon-lattice architecture — IBM Falcon through Condor, 2019–2023 C[72], and Lawrence Berkeley National Laboratory's Advanced Quantum Testbed (AQT) to date — providing entanglement with no coupler control; its alternative is the tunable coupler, and switching is a chip redesign, not firmware. On the derived clock it loses: 180–500 ns against ~50 ns for a tunable-coupler CZ, so every QEC cycle pays 3–7× on the gate layer. Verification: 99.77% is interleaved RB on an isolated pair, blind to spectators; CR error is coherent, so RB understates it and gate-set tomography is the honest measurement.

Actors & economics

Who.
Organisation Role Country What exactly they do Evidence
IBM developer (ex-user) US Invented and scaled CR to Condor; retired it at Heron D[287]
Hanyang University research KR Fixed-frequency lattice-patch design reviving CR S[426]
OQC developer UK Fixed-frequency coaxmons with a fixed-coupling CZ, not CR C[423]

Money.
2026-06-02 · IBM · investment commitment · > $10 B over five years · announced G[57]fact
2026-06-03 · OQC · Series C · £260 M · Bullhound lead · closed C[60]fact

No funding event or QBI stage names cross-resonance.

Market & supply chain. No incremental supplier: the same lithography, cryostat and coax chain, minus per-coupler flux electronics. It paid for G1 and early G2 only.

IP & standards. IBM holds the foundational family (Chow 2011, Kandala 2021); no dated CR-specific patent count was found as of 2026-09-04. Qiskit still ships CR as a native two-qubit template.

Roadmaps & track record. IBM (2022-05-10 · no long-term CR commitment · retired on schedule at Heron, 2023-12 fact). Hanyang (2026-06-25 · simulation only · nothing fabricated). IBM's record is good precisely because it dropped CR when yield turned.

Strategic reading. Nobody wins from CR's supersession except tunable-coupler and cryogenic-control vendors. Its residual value is cheap wiring: if annealing reaches near-unity frequency-targeting yield, a fixed-frequency chiplet undercuts a tunable-coupler chip on cost. Power now sits with the control-electronics vendors — what CR was designed to avoid.

Outlook & open questions

Confirm by 2028: a fabricated fixed-frequency processor above eight qubits with CR fidelity published under simultaneous operation, or the Hanyang patch measured above 98%; else demote to legacy. Best case 2029: a cheap fixed-frequency chiplet; worst case, CR survives only as a Qiskit compilation target. Does anyone outside IBM run CR in production? Does frequency targeting reach collision-free yield past ~100 qubits? Would a foundry pick CR on cost rather than physics?

References
  1. [34] IBM Quantum, “What's new at IBM Quantum - Q2 2026.” [Online]. Available: https://www.ibm.com/quantum/blog/whats-new-q2-2026 D
  2. [57] IBM Quantum, “Why IBM is investing $10 billion into quantum computing,” Jun. 2, 2026. [Online]. Available: https://www.ibm.com/quantum/blog/10-billion-investment-faq G
  3. [60] A. Curbison, “OQC raises £260m in Europe's largest ever private quantum computing funding round,” OQC, Jun. 2, 2026. [Online]. Available: https://oqc.tech/company/newsroom/series-c C
  4. [72] IBM, “Quantum Roadmap.” [Online]. Available: https://www.ibm.com/roadmaps/quantum/ C
  5. [287] A. Kandala et al., “Demonstration of a High-Fidelity CNOT Gate for Fixed-Frequency Transmons with Engineered ZZ Suppression,” Phys. Rev. Lett., vol. 127, no. 13, Art. no. 130501, Sep. 2021, doi: 10.1103/PhysRevLett.127.130501. D
  6. [294] D. P. Pappas et al., “Alternating-bias assisted annealing of amorphous oxide tunnel junctions,” Communications Materials, vol. 5, no. 1, Art. no. 150, Aug. 2024, doi: 10.1038/s43246-024-00596-z. D
  7. [423] A. Curbison, “Oxford research group demonstrate fundamental speed-up of two-qubit gate,” OQC, Mar. 21, 2025. [Online]. Available: https://oqc.tech/company/newsroom/oxford-research-group-demonstrate-fundamental-speed-up-of-two-qubit-gate C
  8. [425] J. M. Chow et al., “Simple All-Microwave Entangling Gate for Fixed-Frequency Superconducting Qubits,” Phys. Rev. Lett., vol. 107, no. 8, Art. no. 080502, Aug. 2011, doi: 10.1103/PhysRevLett.107.080502. D
  9. [426] C. Kim, J. Kang, and Y. Kwon, “Lattice patch structure for fixed-frequency transmon quantum computer with high-fidelity CNOT gates,” arXiv:2606.27017, Jun. 2026. S