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Author: admin

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 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 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.

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 op 60 qubits, deel 1: van Hamiltoniaan naar snake-layout en fSWAPs

Posted on May 12, 2026May 13, 2026 by admin

Een reproduceerbare, kleinere Fermi-Hubbard run laat zien waarom de Q-CTRL aanpak werkt: niet door een generieke compiler, maar door fysica, fermionische mapping, fSWAPs en een hardwarebewuste snake-layout samen te ontwerpen.

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…

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…

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Recent Posts

  • 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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