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
  • 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

XXZham: quantum simulation of 80 spins

NederlandsEnglish

What can a hobbyist investigate with a real quantum computer today? In XXZham, we follow how an ordered pattern of 80 spins changes under their mutual interactions. We use IBM Heron, compare the measured curve with classical calculations, and investigate the role of error mitigation. Our aim is a reproducible NISQ demonstration and a serious research candidate for quantum advantage, not an announcement of proven quantum advantage.

Research status: 21 September 2026. The hardware measurement was performed on 20 September; the classical convergence checks followed on 21 September.

The series

  1. The XXZ model and imbalance

    Spins, the quasiperiodic field, and what we measure.

  2. From dynamics to a quantum circuit

    The interaction picture, Trotter steps, and approximations.

  3. The classical simulation methods

    MPS, TEBD, TDVP, and Pauli propagation.

  4. Error mitigation on real hardware

    TREX, Pauli twirling, XY4, and zero-noise extrapolation.

  5. Results and the classical comparison

    The full trajectory, runtimes, errors, and convergence.

  6. Original study and next steps

    Source code, the Tracker submission, Nighthawk, and candidate status.

OverviewNext: part 1

Recent Posts

  • 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
  • Quantum computing-nieuws — 28 augustus 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