Edukaizen

Menu
  • News
  • Hubbard
    • Hubbard 1D
      • Part 1: 1D Hubbard model
      • Part 2: Snake layout and fSWAP
      • Part 3: Qiskit and Fire Opal
      • Part 4: 120-qubit run
      • Part 5: Time-to-answer
      • Part 6: Tensor networks
      • Part 7: Majorana propagation
      • Part 8: Reading heatmaps
      • Part 9: Digital vs cold-atom labs
      • Part 10: Official Monoprop benchmark
    • Hubbard 2D
      • Part 1: 1D to 2D
      • Part 2: Cuprates
      • Part 3: 3×3
      • Part 4: Time
      • Part 5: 4×4
      • Part 6: 6×6 Fez
    • 2D Local Quantum Advantage
      • Deel 1: Doel en budget
      • Deel 2: Fermionmodel
      • Deel 3: Mapping en diepte
      • Deel 4: Pilots en shots
      • Deel 5: Foutmitigatie
      • Deel 6: 6×6-resultaten
      • Deel 7: Circa 20x
      • Deel 8: Google en Bonsai
      • Deel 9: Volgende stap
  • Hadron
    • Part 1: Hadron on a quantum processor
    • Part 2: Quarks and confinement
    • Part 3: SU(2) and LSH
    • Part 4: Hamiltonian and circuit
    • Part 5: Fire Opal
    • Part 6: Classical simulations
    • Part 7: Quantum advantage
  • Black Hole OLE
    • Part 1: What we ran
    • Part 2: How OLE works
    • Part 3: Fire Opal and Kingston
    • Part 4: The tensor-network challenge
    • Part 5: Hawking and scrambling
    • Part 6: What the result proves
    • Part 7: Local toy model
    • Part 8: QGSS26 compatibility
  • Random Graph
    • Start here
    • Part 1: Theory
    • Part 2: Circuit
    • Part 3: Qiskit
    • Part 4: Complexity
    • Part 5: Verification
    • Part 6: Workflow
    • Part 7: Conclusion
  • Floquet-Ising
    • Part 1: Floquet physics
    • Part 2: Ising cycle
    • Part 3: Two-qubit toy model
    • Part 4: Oscillation and entanglement
    • Part 5: Noise and error mitigation
    • Part 6: Toward 51 qubits
  • XXZham
    • Part 1: The XXZ model and imbalance
    • Part 2: From dynamics to a quantum circuit
    • Part 3: The classical simulation methods
    • Part 4: Error mitigation on real hardware
    • Part 5: Results and the classical comparison
    • Part 6: Original study and next steps
  • Nighthawk RCS 61q
    • Part 1: The paper
    • Part 2: Our IBM measurements
    • Part 3: MPS and advantage
    • Part 4: RCS theory and applications
  • Work
    • QOS QML
      • Tutorial: UMI counts to a four-qubit circuit
      • Part 1: The QML task
      • Part 2: QOS theory
      • Part 3: Gene expression to 40 qubits
      • Part 4: JAX to hardware
      • Part 5: Readout and classifier
      • Part 6: 40-qubit result
      • Part 7: Route to quantum advantage
      • Part 8: 60-qubit result
    • Quantum Gold
      • Part 1: Why gold is a relativistic quantum problem
      • Part 2: Why the 2025 gold VQE study stalled
      • Part 3: From QE and spin–orbit coupling to Qiskit
      • Part 4: Twelve gold spinor modes on four qubits
      • Part 5: The 24-qubit route: an active window for transport
      • Part 6: 24 qubits on IBM and with Fire Opal
      • Part 7: The road to quantum advantage for gold
      • Part 8: 24 gold spinor modes on IBM with ZNE-PEA
      • Part 9: Forced gold colour on 56 qubits
    • HaPPY Gravity
      • Part 1: Gravity as a phase gate
      • Part 2: Bosons and convergence
      • Part 3: The dynamic HaPPY benchmark
      • Part 4: The N=145 classical audit
      • Part 5: MPS and Majorana baselines
      • Part 6: PEA/ZNE and the decisive test
    • Fibonacci Anyons
      • Part 1: Fusion and braiding
      • Part 2: The 3/5/9-qubit ladder
      • Part 3: Why nine qubits were too deep
      • Part 4: Structure-aware simplification
      • Part 5: IBM hardware diagnostic
      • Part 6: Results and open questions
  • Advantage List
  • Contact
Menu

Part 2: Our million 61-qubit measurements on IBM

Nederlands

We executed the released circuit again on ibm_phoenix with a hard 60-second QPU execution cap. The job completed with 19 QPU seconds.

The new hardware job

On 25 September 2026 we sent the released 61-qubit, 36-cycle circuit to ibm_phoenix. It used the same logical gates and published physical layout, with 918 CZ gates after compilation. One IBM SamplerV2 job contained ten blocks of 100,000 shots. Measurement twirling was enabled; max_execution_time was set to 60 seconds. Job dar90plvr3kc73eij3vg finished with one million outcomes and 19 seconds of QPU usage. The circuit-execution field reported 15.127 seconds; submission-to-completion took more than seven minutes. These are different clocks.

What do the outcomes contain?

Each outcome is one string of 61 zeros and ones. All million observed strings were distinct. They contained an average of 30.440323 ones. The paper’s published million strings contained 30.423606 ones on average. The total-variation distance between the two histograms of the total number of ones was 0.003272. Across the 61 individual bit positions, the root-mean-square difference in P(bit=1) was about 0.002092.

Those are concrete agreements in simple statistics. They do not tell us whether outcomes with high ideal probabilities occur more often. Two very different 61-bit distributions can share the same number-of-ones histogram.

What we did and did not repeat

We repeated the scale, circuit, shot count and 19-second QPU timing. We did not run a full new mirror-and-patch series. We therefore do not assign the paper’s approximate 0.0023 fidelity to our new million bitstrings. A separate 21-qubit patch pilot gave IBM XEB about 0.313 and a Fire Opal point estimate about 0.385; that smaller patch does not measure full-circuit quality.

The paper repository contains the original circuit and published raw measurements. Our new job ID and figures are recorded above; the new raw outcomes remain in our local qlab project.

Original preprint

Project overview and article source

Previous · Next · Overview

Edukaizen · 25 september 2026 / 25 September 2026

Recent Posts

  • Quantum computing-nieuws — 25 september 2026
  • Quantum computing-nieuws — 18 september 2026
  • A Call to Qiskit Advocates: Help Test Quantum Advantage
  • Quantum computing-nieuws — 11 september 2026
  • Quantum computing-nieuws — 4 september 2026

Recent Comments

  1. XXZham: simulating 80 spins with a NISQ quantum computer - Edukaizen on XXZham: quantumsimulatie van 80 spins

Archives

  • September 2026
  • August 2026
  • July 2026
  • May 2026
  • March 2026
  • February 2026
  • September 2024

Categories

  • 10
  • Quantum Computing
  • Uncategorized
©2026 Edukaizen | Theme by SuperbThemes