Edukaizen

Menu
  • News
  • 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
  • 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
  • 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
  • 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
  • Work
    • 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
Menu

Black Hole OLE, part 4: the tensor-network challenge

Posted on July 11, 2026July 20, 2026 by admin
Black Hole OLE series | Series page | Previous | Next

The phrase "quantum advantage" is not earned by running a large circuit. A serious claim needs a strong classical competitor, an accuracy target, and honest timing boundaries.

For this project, the classical competitor was not a generic statevector simulator. It was the tracker-linked TensorNetworkQuantumSimulator.jl route, which evolves the ZZZ operator in the Heisenberg picture using belief propagation and bond-dimension truncation.

That is a natural competitor because the quantum task asks for one observable, not the entire 80-qubit wavefunction.

Validating the runner first

Before attempting Q80, the new Julia runner was tested against an existing six-qubit tracker BP-TN artifact at bond dimension 64. It reproduced the stored observable to an absolute difference of 1.1e-16 and the pre-rescale norm to 2.3e-18.

That regression establishes that the gate reversal, CZ decomposition, local tensor normalization, and final overlap follow the prior tracker implementation.

The Q80 convergence ladder

At bond dimension 16, both halves completed:

  • Delta: 0.40925590, wall time 209.21 seconds, truncation sum 4.12081
  • Delta zero: 0.41780650, wall time 155.93 seconds, truncation sum 3.80119
  • Apparent ratio: 0.97953456

That ratio is not trustworthy. The truncation errors are too large.

At bond dimension 32, the delta value moved to 0.76129858 with a truncation sum of 1.32017. The change from bond dimension 16 was 0.35204, or 86 percent. This shift is more than twenty times the hardware standard error.

At bond dimension 64, the delta half did not produce a result within a hard 900-second limit. A complete ratio would still require the delta-zero half and then a higher-bond convergence check.

Is the quantum computer faster?

For this tested local implementation, yes. The complete mitigated 16-circuit Fire Opal action finished in 328 seconds. The classical BD64 delta half alone exceeded 901 seconds. That gives an observed end-to-end lower bound above 2.75x for this machine and workflow.

Compared only with the 43.85-second QPU usage estimate, the observed lower bound is above 20.55x. That number is less fair as an end-to-end comparison because it excludes managed quantum overhead.

Why this is not yet a universal advantage claim

The classical result has not converged to the quantum error scale. We also have not benchmarked every classical algorithm, GPU implementation, distributed tensor contraction, or optimized compute node.

The supported statement is narrower:

The Q80 hardware workflow produced its finite-sample observable within minutes, while the tested tracker BP-TN route did not reach a controlled higher-bond answer within the same time scale.

That is evidence of a local practical runtime advantage, sometimes called a time-to-answer advantage. It is not proof that all classical computers fail on all formulations of the task.

This nuance becomes especially important when we connect OLE to information scrambling and black holes. A beautiful physical analogy should make our standards stronger, not weaker.

Sources

  • TensorNetworkQuantumSimulator.jl
  • Tracker OLE model and released circuits
Black Hole OLE series | Series page | Previous | Next

Recent Posts

  • Quantum computing-nieuws — 21 augustus 2026
  • Quantum computing-nieuws — 20 augustus 2026
  • Quantum computing-nieuws — 19 augustus 2026
  • Quantum computing-nieuws — 18 augustus 2026
  • Quantum computing-nieuws — 17 augustus 2026

Recent Comments

No comments to show.

Archives

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

Categories

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