Skip to content

Quantum Energy Teleportation

Quantum energy teleportation (QET) is a correlation-assisted local-energy extraction protocol. A measurement in region AA injects energy and produces a classical outcome; after that outcome reaches region BB, a conditional local operation can extract energy there. No energy or information propagates outside the light cone, and “teleportation” does not mean that the extracted energy traveled from AA to BB.

Required background. Passivity and work fixes the energy reference, measurement energy and backreaction supplies the instrument account, and quantum energy inequalities constrain regulated local energy profiles.

Helpful background. Entanglement harvesting distinguishes use of pre-existing correlations from causal energy exchange.

Let {Ma}\{M_a\} be a localized instrument in AA, with outcome probability pap_a, and let UaBU_a^B be a local unitary in BB chosen after receiving aa. The averaged final state is

ρf=aUaBMaρ0MaUaB.\rho_f=\sum_a U_a^B M_a\rho_0 M_a^\dagger U_a^{B\dagger}.

With a fixed Hamiltonian HH, define measurement injection

EA=atr(HMaρ0Ma)tr(Hρ0)E_A=\sum_a\operatorname{tr}(H M_a\rho_0M_a^\dagger) -\operatorname{tr}(H\rho_0)

and remote extraction

EB=atr ⁣[H(Maρ0MaUaBMaρ0MaUaB)].E_B=\sum_a\operatorname{tr}\!\left[ H\left(M_a\rho_0M_a^\dagger- U_a^B M_a\rho_0M_a^\dagger U_a^{B\dagger}\right) \right].

A successful protocol has EB>0E_B>0 while respecting the causal delay for the classical message. Local passivity can forbid extraction by an outcome-independent operation at BB even though correlations make the conditioned operation effective. Hotta 2010, §§ 2–4 develops this mechanism in regulated spin and field models.

Start with a finite harmonic chain approximating a scalar field ground state. Choose separated blocks AA and BB, a finite-resolution Gaussian measurement in AA, and an outcome-dependent displacement in BB. Optimize UaBU_a^B using the conditional first moments and covariance. Report:

  • EAE_A, EBE_B, controller and message costs;
  • the separation and earliest allowed feed-forward time;
  • the result with the AABB covariance set to zero;
  • lattice-spacing, volume, and measurement-resolution convergence.

If the message is removed, average over an outcome-independent UBU^B and verify that the claimed extraction disappears. If the initial correlations are removed while local marginals are matched, the advantage should disappear. These are stronger causal controls than observing EB>0E_B>0 once.

Separate hypothesis chains lead from cyclic dynamics to passivity, sampled stress energy to QEI or ANEC, modular data to an entropy–energy bound, null shape variation to QNEC, and localized instruments to cost or QET.

QET joins the localized-instrument branch to passivity and a complete energy account. The relevant resource is the conditional correlation structure; the classical message controls a local extraction operation. The diagram is schematic.

Before the message reaches BB, the reduced statistics of every operation in BB are independent of aa. The final local negative-energy region is balanced by the measurement injection, subsequent propagation, and positive energy elsewhere according to the model’s dynamics and applicable energy inequalities. Correlation alone is not sufficient: the instrument and conditional operation must couple to it in the right way.

A proposed bound passes through independent checks of operator domain, averaging geometry, renormalization and species, and full operational energy accounting; omissions lead to four distinct false conclusions.

Calling the protocol superluminal, identifying correlation with transported energy, or omitting measurement injection and feed-forward cost are distinct errors. The map is schematic.

As of 10 August 2026, QET has rigorous and numerical realizations in finite spin, oscillator, and field-theory models. Quantum processors have executed circuits representing small QET Hamiltonians, including Ikeda 2023, “Superconducting Quantum Hardware,” §§ II–IV, and field-theory simulations have explored critical enhancement in the massive Thirring model Ikeda 2023, “Criticality,” §§ II–IV. These results do not yet demonstrate spatially separated continuum-field energy extraction in a laboratory; hardware simulation of a model and direct measurement of a field protocol are different evidence classes.

  • Hotta, Masahiro. “Quantum Energy Teleportation: An Introductory Review.” Journal of Physics A: Mathematical and Theoretical 43 (2010): 105305. DOI.
  • Ikeda, Kazuki. “Criticality of Quantum Energy Teleportation at Phase Transition Points in Quantum Field Theory.” Physical Review D 107 (2023): L071502. DOI.
  • Ikeda, Kazuki. “Demonstration of Quantum Energy Teleportation on Superconducting Quantum Hardware.” Physical Review Applied 20 (2023): 024051. DOI.