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    • Part 1: 1D Hubbard model
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    • Part 1: 1D to 2D
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  • Quantum Tracker OLE Q80
    • 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
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Quantum Tracker OLE Q80, part 5: Hawking, black holes, and scrambling

Posted on July 11, 2026 by admin

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

Quantum Tracker OLE Q80, part 6: what the result proves and what comes next

Posted on July 11, 2026 by admin

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

Quantum Tracker OLE Q80, part 4: the tensor-network challenge

Posted on July 11, 2026 by admin

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

Quantum Tracker OLE Q80, part 3: Fire Opal on IBM Kingston

Posted on July 11, 2026 by admin

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

Quantum Tracker OLE Q80, part 1: what we actually ran

Posted on July 11, 2026 by admin

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

Quantum Tracker OLE Q80, part 2: how an Operator Loschmidt Echo works

Posted on July 11, 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.

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Recent Posts

  • Quantum Tracker OLE Q80, part 6: what the result proves and what comes next
  • Quantum Tracker OLE Q80, part 5: Hawking, black holes, and scrambling
  • Quantum Tracker OLE Q80, part 4: the tensor-network challenge
  • Quantum Tracker OLE Q80, part 3: Fire Opal on IBM Kingston
  • Quantum Tracker OLE Q80, part 2: how an Operator Loschmidt Echo works

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