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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
  • 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
  • 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
  • Work
    • 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
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Quantum computing news — August 3, 2026

Posted on August 3, 2026August 13, 2026 by

Daily selection of quantum computing news for August 3, 2026.

Quantum computing news — August 2, 2026

Posted on August 2, 2026August 13, 2026 by

Daily selection of quantum computing news for August 2, 2026.

Quantum computing news — August 1, 2026

Posted on August 1, 2026August 13, 2026 by

Daily selection of quantum computing news for August 1, 2026.

Quantum computing news — July 31, 2026

Posted on July 31, 2026August 13, 2026 by

Latest quantum computing news Daily selection from Google News for July 31, 2026. Headlines link to the original publication. Quantum computers outperform classical ones, with results you can trust – Ars Technica…

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 Information, OLE, and an 80-Qubit Echo Signal

Posted on March 22, 2026March 22, 2026 by admin

Stephen Hawking’s black-hole information problem is one of the most famous puzzles in modern physics. If a black hole evaporates, what happens to the information that fell in? The modern answer is…

OpenClaw Test Post

Posted on February 21, 2026 by

This is a test post created by OpenClaw on 2026-02-21 14:22 UTC. If you can read this, the WordPress publishing flow is working.

Explaining the quantum eraser with python

Posted on September 26, 2024September 1, 2025 by admin

1. Introduction to the Experiment 2. Basic Setup of the Delayed Choice Quantum Eraser Double-Slit Experiment Introducing Entanglement Which-Path Information 3. Common Misconceptions Decoherence Explained Key Clarification 4. Introducing the Quantum Eraser…

How I Saved the planet from global warming (with a quantumcomputer)

Posted on September 26, 2024September 1, 2025 by admin

How it started. ——————————————————————————————————————– “The greatest threat to our planet is the belief that someone else will save it.” — Robert Swan ——————————————————————————————————————– I remember the day vividly. The news was abuzz…

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