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  • 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
  • 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
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  • Random Graph
    • Part 1: Theory
    • Part 2: Circuit
    • Part 3: Qiskit
    • Part 4: Complexity
    • Part 5: Verification
    • Part 6: Workflow
    • Part 7: Conclusion
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Fermi-Hubbard on a quantum computer, part 9: why 2D Hubbard is the real next boundary

Posted on July 2, 2026 by

English | Nederlands | Project page | Previous The 1D Fermi-Hubbard chain is a good testbed. But the bigger physics ambition is in 2D. Why? Because the 2D Hubbard model is much…

Fermi-Hubbard on a quantum computer, part 8: heatmaps as a material-like measurement

Posted on July 2, 2026 by

English | Nederlands | Project page | Previous | Next A table of RMSE values is useful, but it is not a physical picture. For a material-like story, we want to see…

Fermi-Hubbard on a quantum computer, part 7: Majorana propagation as a laptop competitor

Posted on July 2, 2026July 2, 2026 by admin

English | Nederlands | Project page | Previous | Next A good quantum-advantage discussion needs a strong classical competitor. In this series, tensor-network TDVP is the standard competitor, but there is another…

Fermi-Hubbard on a quantum computer, part 6: tensor networks, TDVP, and chi

Posted on July 2, 2026 by

English | Nederlands | Project page | Previous | Next If we want to benchmark a quantum computer, we need a strong classical competitor. For 1D quantum chains, that competitor is usually…

Fermi-Hubbard on a quantum computer, part 5: quantum advantage or time-to-answer?

Posted on July 2, 2026 by

English | Nederlands | Project page | Previous | Next "Quantum advantage" is a dangerous phrase. It sounds absolute: the quantum computer wins and the classical computer loses. For near-term many-body simulation,…

Fermi-Hubbard on a quantum computer, part 4: the 120-qubit quantum run

Posted on July 2, 2026 by

English | Nederlands | Project page | Previous | Next Now we reach the question that motivates this project: what happens when we run the Fermi-Hubbard simulation on real quantum hardware? The…

Fermi-Hubbard on a quantum computer, part 3: Qiskit, IBM Runtime, and Fire Opal

Posted on July 2, 2026 by

English | Nederlands | Project page | Previous | Next The first two parts were about the physics and the circuit structure. This part is about the practical route: how do we…

Fermi-Hubbard op een quantumcomputer, deel 2: snake layout en fSWAP

Posted on July 2, 2026July 2, 2026 by

Nederlands | English | Project page | Previous | Next Een Fermi-Hubbard Hamiltoniaan is nog geen quantumcircuit. Eerst moeten de fermionische modes naar qubits worden vertaald. Daarna moet het circuit op een…

Fermi-Hubbard on a quantum computer, part 2: snake layout and fSWAP

Posted on July 2, 2026July 2, 2026 by

English | Nederlands | Project page | Previous | Next A Fermi-Hubbard Hamiltonian is not yet a quantum circuit. First, the fermionic modes must be mapped to qubits. Then the circuit must…

Fermi-Hubbard on a quantum computer, part 1: the 1D Hubbard model

Posted on July 2, 2026July 2, 2026 by

English | Nederlands | Project page | Next This project does not start with qubits. It starts with a physical model: the one-dimensional Fermi-Hubbard model. The model describes fermions that can hop…

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  • Black Hole OLE, part 7: a local toy model with theory and user guide
  • Black Hole OLE, part 6: what the result proves and what comes next
  • Black Hole OLE, part 5: Hawking, black holes, and scrambling
  • Black Hole OLE, part 4: the tensor-network challenge
  • Black Hole OLE, part 3: Fire Opal on IBM Kingston

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