Showcase #4 · Batch #2
Quantum Thermodynamics

Quantum Vacuum Measurement Engine

A quantum engine whose working medium is the coupling-deformed vacuum itself.

Czupryniak, Bhandari, Erdman, Jordan (2026)arXiv
Quantum Vacuum Measurement Engine

Full engine thermodynamics across the coupling sweep: work W(λ), measurement heat Q(λ), and efficiency η(λ). Numerical dots from the 8-point 6-step cycle sit exactly on the analytical curves.

W = 0.293
Work per cycle at β = λ = 1, matching the paper's closed-form to 6 × 10⁻⁵

[ overview ]

What this reproduces & why it matters

Czupryniak et al. (2026) — a fresh 2026 preprint from Andrew Jordan's group — defines a Quantum Vacuum Measurement Engine (QVME): a genuine thermodynamic engine that extracts work from the coupling-induced deformation of a quantum many-body ground state.

Every thermodynamic scalar of the engine — work per cycle W, measurement heat input Q, efficiency η — is a derivative of a single geometric quantity: the Quantum Vacuum Bending Function Δ(λ) = E₀(0) − E₀(λ). This showcase reproduces the paper's 2-qubit worked example end-to-end and demonstrates the full 6-step engine cycle.

[ verified results ]

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

verified
VQE ground state error vs. −√(β² + λ²)
every coupling in the sweep
< 10⁻⁶
Canonical benchmark W(1) numerical vs. analytical
W_num = +0.29295, W_ana = +0.29289
6 × 10⁻⁵ error
Coupling sweep pass rate
tolerance 10⁻³, all points
8/8 PASS
Analytical efficiency η(1)41.4%
ZNE mitigation improvement (avg over sweep)
up to 6.4× at strong coupling
3.0×

[ method ]

How it's built

Hamiltonian H(λ) = (β/2)(Z₀ + Z₁) + λ · X₀X₁ (paper Sec. II worked example). Ground state via VQE with a parity-preserving RY + CX ansatz — the same 2-qubit subspace where H₂ lives (see Showcase #5). Full 6-step cycle: init → Z-basis measurement → quench λ off → coherent work extraction → quench λ on → thermal relaxation.

Coupling sweep at 8 points from λ = 0.2 to λ = 3.0 verifies numerical work per cycle against the closed-form W(λ) = β − β²/√(β² + λ²).

[ circuit ]

The actual Qiskit circuit

hardware-buildable
6-step QVME engine cycle circuit

Schematic dynamic-circuit implementation of the 6-step engine cycle: init |0(λ)⟩ → Z-basis measure → quench off → conditional work extraction → quench on → relax.

[ figures ]

Physics visuals

QVBF Δ(λ) landscape
The Quantum Vacuum Bending Function Δ(λ) = √(β² + λ²) − β and its derivative Δ'(λ). This is the central geometric object of the entire engine theory — every thermodynamic scalar is a derivative of it.
ZNE recovery of the work curve under Heron noise
Under real Heron noise, ZNE recovery scales with signal-to-noise ratio: 1.4× at λ = 0.5, up to 6.4× at λ = 2.0. Richardson ZNE's expected behavior visible directly in the data.

[ mitigation ]

What Qubital's ZNE buys you here

The 2-qubit shallow ansatz stays well inside the linear-response regime of Richardson ZNE at every coupling. Recovery averages 3.0× across the sweep, peaking at 6.4× at strong coupling where the noiseless signal dominates the noise floor.

[ references ]

Papers & sources

  • Czupryniak, R., Bhandari, B., Erdman, P. A., Jordan, A. N. (2026). "Universal Characterization of Quantum Vacuum Measurement Engines."
  • Elouard, C., Herrera-Martí, D., Huard, B., Auffèves, A. (2017). "Extracting Work from Quantum Measurement in Maxwell's Demon Engines." Phys. Rev. Lett. 118, 260603.
  • Bhandari, B., Czupryniak, R., Erdman, P. A., Jordan, A. N. (2023). "Measurement-Based Quantum Thermal Machines with Feedback Control." Entropy 25, 204.

[ what's next ]

Roadmap for this showcase

roadmap
  • Multi-cycle work extraction — chain the 6-step cycle over N iterations and verify aggregate W = N · W(λ) with drift analysis under noise
  • Coupling-sweep hardware run on real Heron r2 once IBM access is restored
  • Extend to the paper's 4-qubit and N-qubit variants

[ request access ]

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