Edukaizen

Menu
  • Home
  • 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
  • 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
  • Advantage List
Menu

Fermi-Hubbard op een quantumcomputer, deel 10: kan een quantumcomputer een quantumlab vervangen?

Posted on July 27, 2026July 27, 2026 by admin

Cold atoms en gate-based processors kunnen dezelfde 1D Fermi-Hubbarddynamica onderzoeken, maar vervanging van een quantumlab vereist dezelfde Hamiltoniaan, begintoestand, quench, observabelen en validatie.

Fermi-Hubbard on a quantum computer, part 10: can a quantum computer replace a quantum lab?

Posted on July 27, 2026July 27, 2026 by admin

Cold atoms and gate-based processors can probe the same 1D Fermi-Hubbard dynamics, but replacing a quantum lab requires matching the Hamiltonian, initial state, quench, observables, and validation.

Black Hole OLE, part 8: QGSS26 and protocol compatibility

Posted on July 25, 2026 by

Black Hole OLE series | Series page | Previous The Operator Loschmidt Echo (OLE) was one of the observable-estimation examples discussed by Minh Tran in Quantum Algorithms III at the Qiskit Global…

Black Hole OLE, part 7: a local toy model with theory and user guide

Posted on July 22, 2026July 25, 2026 by

Black Hole OLE series | Series page | Previous | Next The 80-qubit experiment is the main result of this series, but it is not the easiest place to learn what an…

Black Hole OLE, part 5: Hawking, black holes, and scrambling

Posted on July 11, 2026July 20, 2026 by admin

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

Black Hole OLE, part 6: what the result proves and what comes next

Posted on July 11, 2026July 22, 2026 by admin

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

Black Hole OLE, part 4: the tensor-network challenge

Posted on July 11, 2026July 20, 2026 by admin

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

Black Hole OLE, part 3: Fire Opal on IBM Kingston

Posted on July 11, 2026July 20, 2026 by admin

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

Black Hole OLE, part 1: what we actually ran

Posted on July 11, 2026July 20, 2026 by admin

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

Black Hole OLE, part 2: how an Operator Loschmidt Echo works

Posted on July 11, 2026July 20, 2026 by admin

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

  • 1
  • 2
  • 3
  • 4
  • Next

Recent Posts

  • Fermi-Hubbard op een quantumcomputer, deel 10: kan een quantumcomputer een quantumlab vervangen?
  • Fermi-Hubbard on a quantum computer, part 10: can a quantum computer replace a quantum lab?
  • Black Hole OLE, part 8: QGSS26 and protocol compatibility
  • 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

Recent Comments

No comments to show.

Archives

  • July 2026
  • May 2026
  • March 2026
  • February 2026
  • September 2024

Categories

  • 10
  • Quantum Computing
  • Uncategorized
©2026 Edukaizen | Theme by SuperbThemes