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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: 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
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    • 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
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    • 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
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    • Start here
    • Part 1: Theory
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    • Part 4: Complexity
    • Part 5: Verification
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    • 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
  • GOLD REL
    • 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
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Month: July 2026

Black Hole OLE, part 1: what we actually ran

Posted on July 11, 2026August 9, 2026 by admin

A reproducible Q80 Operator Loschmidt Echo study, from circuit construction and hardware execution to tensor-network limits and information scrambling.

Fermi-Hubbard 2D cuprate series, part 6: 6×6 tensor baseline, IBM diagnostics, and Fire Opal Fez

Posted on July 4, 2026 by

The 6×6 step reaches 72 qubits, but the current hardware result is still diagnostic: Fire Opal Fez improves strongly over IBM, while sector survival remains low.

Fermi-Hubbard 2D cuprate series, part 5: 4×4 hardware and tensor baselines

Posted on July 4, 2026 by

The 4×4 run is where exact ED stops being the comfortable reference route and tensor baselines become necessary.

Fermi-Hubbard 2D cuprate series, part 4: time evolution and hardware diagnostics

Posted on July 4, 2026 by

The 3×3 hardware comparison shows the main diagnostic pattern: Fire Opal is cleaner than direct IBM, but sector survival still falls with time.

Fermi-Hubbard 2D cuprate series, part 3: our 3×3 implementation

Posted on July 4, 2026 by

The 3×3 run is not meant to be large-scale cuprate physics. It is the exact validation lab that makes the later hardware results interpretable.

Fermi-Hubbard 2D cuprate series, part 2: 2D Hubbard, cuprates, and Google/Willow context

Posted on July 4, 2026July 4, 2026 by

The 2D route is motivated by the one-band Hubbard model as a minimal description of strongly correlated electrons in cuprate-like planes.

Fermi-Hubbard 2D cuprate series, part 1: from 1D to 2D

Posted on July 3, 2026July 4, 2026 by

The second Fermi-Hubbard series starts by carrying the validation discipline from the earlier 1D IBM/TDVP route into a 2D cuprate-oriented ladder.

Van Hubbard 1D naar de Hubbard 2D-serie

Posted on July 2, 2026August 11, 2026 by

Nederlands | English | Hubbard 1D-project | Verder met Hubbard 2D Update van de reeks: deze pagina was oorspronkelijk de 2D-outlook van de Hubbard 1D-reeks. Het 2D-werk heeft inmiddels een eigen, uitgebreidere…

Fermi-Hubbard op een quantumcomputer, deel 8: charge- en spinheatmaps lezen

Posted on July 2, 2026August 11, 2026 by

Nederlands | English | Project page | Previous | Next Reikwijdte van dit deel: dit deel legt uit hoe je de charge- en spinheatmaps leest. Deel 9 gebruikt die observabelen voor een…

Fermi-Hubbard op een quantumcomputer, deel 7: Majorana propagation als laptop-tegenstander

Posted on July 2, 2026 by

Nederlands | English | Project page | Previous | Next Een goede quantum-advantage discussie heeft een sterke klassieke tegenstander nodig. Voor deze reeks is tensor-network TDVP de standaardtegenstander, maar er is nog…

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