Edukaizen

Menu
  • Nieuws
  • 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: Heatmaps
    • Part 9: 2D Hubbard outlook
    • Part 10: Quantum computer as a lab
    • Part 11: 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
    • Deel 1: Hadron op quantumprocessor
    • Deel 2: Quarks en confinement
    • Deel 3: SU(2) en LSH
    • Deel 4: Hamiltoniaan en circuit
    • Deel 5: Fire Opal
    • Deel 6: Klassieke simulaties
    • Deel 7: Quantumvoordeel
  • 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
    • Nederlands
    • English
    • Beginnershandleiding 4q
  • 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
  • Quantumgoud
    • Deel 1: Waarom goud een relativistisch quantumprobleem is
    • Deel 2: Waarom het goud-VQE-onderzoek uit 2025 vastliep
    • Deel 3: Van QE en spin-baan-koppeling naar Qiskit
    • Deel 4: Twaalf goud-spinormodi op vier qubits
    • Deel 5: De 24-qubit route: een actief venster voor transport
    • Deel 6: 24 qubits op IBM en met Fire Opal
    • Deel 7: De route naar quantumvoordeel voor goud
  • Advantage List
Menu

The 24-qubit route: an active window for transport

NederlandsEnglish

Part 5 · 24-qubit algorithm

For 24 qubits we did not start with a large circuit and invent a story afterwards. We selected one local question: how much of a short domain-wall imbalance remains after 0.10 femtoseconds?

The active window

The model has four sites, six fermionic modes per site and twelve electrons. The central observable compares occupations on both sides of the middle and ranges from −1 to 1. Exact evolution gives an imbalance of 0.9872906000 at 0.10 fs.

A two-site window gives 0.9872156850. Their difference, 0.000074915, is below the predeclared threshold of 0.001, while the norm error also remains far below its threshold. This validates the four-site window for this observable and time—not automatically for spectra, longer times or the complete state.

Observable-specific first order

A first-order product formula does deviate globally from the exact state: at 12 qubits the state fidelity is 0.986226. Nevertheless, the error in the selected imbalance is only 0.000400 at 12 qubits and 0.000382 at 24 qubits. This illustrates why an observable-specific criterion can be sharper than demanding that the entire wavefunction be almost exact.

Routing 24 qubits

The frozen route transpiled for IBM Kingston to depth 632 with 693 CZ gates, passing the predeclared screens of depth at most 1000 and at most 2000 two-qubit gates. The experiment measures twelve central modes rather than reconstructing the full state.

Important: this 24-qubit Hamiltonian is Au-inspired. It includes s–d orbital structure, scalar-relativistic shifts, spin–orbit coupling, interactions and orbital-dependent hopping, but has not yet been imported from the validated QE/Wannier matrices.
Claim boundary. Validation applies only to the central imbalance at 0.10 fs. It does not approve the global state, other observables, gold optics or a quantum advantage claim.
Project page: Relativistic gold

  1. Part 1: Why gold is a relativistic quantum problem
  2. Part 2: Why the 2025 gold VQE study stalled
  3. Part 3: From QE and spin–orbit coupling to Qiskit
  4. Part 4: Twelve gold spinor modes on four qubits
  5. Part 5: The 24-qubit route: an active window for transport
  6. Part 6: 24 qubits on IBM and with Fire Opal
  7. Part 7: The road to quantum advantage for gold

Sources and reproducibility

  • Hubbard’s original model
  • IBM Qiskit: PauliEvolutionGate

Project status: 8 August 2026. Numerical values come from the frozen local research artifacts; the original claim boundaries are deliberately preserved.

Recent Posts

  • Quantum computing-nieuws — 8 augustus 2026
  • Quantum computing-nieuws — 7 augustus 2026
  • Quantum computing-nieuws — 6 augustus 2026
  • Quantum computing-nieuws — 5 augustus 2026
  • Quantum computing-nieuws — 4 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