Showcase #1 · Batch #1
Quantum Information Theory

Quantum Energy Teleportation

Alice sends Bob one classical bit. Bob extracts negative energy.

Ikeda (2023) — First hardware realization of QET on IBMarXiv
Quantum Energy Teleportation

Bob's local energy sweep. At the optimal conditional rotation θ* = π/2, Bob's subsystem drops to exactly −1.000 — below the vacuum ground-state energy — funded by pre-existing entanglement and one classical bit.

−1.000
Bob's local energy — a full unit below the vacuum

[ overview ]

What this reproduces & why it matters

Hotta's 2008 Quantum Energy Teleportation protocol shows that when two observers share the ground state of an interacting Hamiltonian, one can "teleport" locally-accessible energy by measuring their half and sending the outcome as a single classical bit. The receiver applies a conditional rotation and — impossibly, at first glance — extracts a negative amount of local energy while global energy conservation is preserved by the exchange.

Ikeda's 2023 IBM hardware demonstration confirmed the protocol experimentally. This showcase reproduces the full protocol on a 2-qubit ground state, verifies Bob's optimum matches the analytical θ = π/2, and demonstrates that Qubital's ZNE mitigation recovers the fragile negative-energy signature with 632× less error than raw Heron-scale noise.

[ verified results ]

Every number below is [PASS]-checked in source.

verified
VQE convergence error vs. exact ground state6.2 × 10⁻⁶
Bob's local energy at optimum θ* = π/2
matches analytical prediction exactly
−1.000
ZNE improvement at Heron scale
raw noise error / ZNE-recovered error
632×

[ method ]

How it's built

VQE preparation of the 2-qubit interacting ground state (RY–CX–RY ansatz, 4 parameters, SPSA optimizer). Alice performs a projective Z-measurement on qubit 0 and sends the outcome as a classical bit. Bob applies a conditional rotation R_Y(±θ) on qubit 1 and Qubital reads out ⟨H_B⟩ = h⟨X_1⟩ via an X-basis measurement.

For the mitigation demo, we deliberately amplify device noise, apply global circuit folding at fold factors {1×, 3×, 5×}, and use Richardson linear extrapolation to recover the noiseless value at scale = 0.

[ circuit ]

The actual Qiskit circuit

hardware-buildable
Dynamic circuit implementation of the QET protocol

The full dynamic-circuit implementation: shared ground state prep → Alice's projective Z-measurement → classical feedback → Bob's conditional rotation → X-basis readout.

[ figures ]

Physics visuals

VQE convergence trajectory for the 2-qubit QET ground state
VQE + SPSA converges to the exact ground-state energy within 6.2 × 10⁻⁶ over 300 iterations. The 4-parameter ansatz has zero residual variational error.
Richardson ZNE recovery of Bob's negative-energy signal
Under amplified NISQ noise, Bob's ⟨H_B⟩ drifts from the −1.000 target. Global circuit folding at three noise scales + Richardson linear extrapolation to scale = 0 recovers the negative-energy signature with 632× less error.

[ mitigation ]

What Qubital's ZNE buys you here

The QET negative-energy signal is one of the most fragile physical signatures ever measured on a NISQ device. Qubital's Richardson linear ZNE reduces the recovery error by 632× at real Heron noise — the largest single-showcase improvement factor in the library.

[ references ]

Papers & sources

  • Hotta, M. (2008). "A Protocol for Quantum Energy Distribution." Physics Letters A 372.
  • Ikeda, K. (2023). "Realization of Quantum Energy Teleportation on Superconducting Quantum Hardware."
  • Temme, K., Bravyi, S., Gambetta, J. M. (2017). "Error Mitigation for Short-Depth Quantum Circuits." Phys. Rev. Lett. 119, 180509.
    arXivRichardson ZNE method

[ what's next ]

Roadmap for this showcase

roadmap
  • Scale to the 6-qubit XXZ chain extension of QET (Ikeda + Yusa 2024)
  • Run the dynamic circuit on real Heron r2 hardware once IBM access is restored
  • Compare linear ZNE vs. exponential ZNE at moderate noise scales for this ansatz

[ request access ]

Want to run this yourself?

The physics-showcases repo is currently private, protecting IP pre-revenue. Physicists, quantum-industry contacts, and investors: reach out and I'll set up a technical walkthrough, call, or Loom.

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