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Nontrivial bounds on extractable energy in quantum energy teleportation for gapped manybody systems with a unique ground state

Taisanul Haque

TL;DR

This work proves a universal, nonperturbative upper bound on the net energy extractable via Quantum Energy Teleportation (QET) in finite-range gapped lattice systems with a unique ground state: the energy difference between sender and receiver obeys $|E_A-E_B|\le C e^{-\mu d}$, where $d$ is the separation and $C,\mu$ are set by the spectral gap, interaction range, and local operator norms. The authors combine a variational reduction with exponential clustering (via Lieb-Robinson bounds and the gap) and a careful local-decomposition analysis to bound cross-region correlations, showing that local measurements perturb the ground state only in a finite neighbourhood and that classical communication cannot overcome this to achieve substantial energy transfer at large $d$. A refinement using commutator structure of decoding unitaries yields potentially tighter prefactors when $U_a$ has a local generator. The results provide rigorous justification for the locality of QET effects and offer a route to compute explicit constants for specific models, with potential extensions to thermal states and more general quantum operations.

Abstract

We establish a universal, exponentially decaying upper bound on the average energy that can be extracted in quantum energy teleportation (QET) protocols executed on finite-range gapped lattice systems possessing a unique ground state. Under mild regularity assumptions on the Hamiltonian and uniform operator-norm bounds on the local measurement operators, there exist positive constants $C$ and $μ$ (determined by the spectral gap, interaction range and local operator norms) such that for any local measurement performed in a region $A$ and any outcome-dependent local unitaries implemented in a disjoint region $B$ separated by distance $d=\operatorname{dist}(A,B)$ one has $|E_A-E_B|\le C\,e^{-μd}.$ The bound is nonperturbative, explicit up to model-dependent constants, and follows from the variational characterization of the ground state combined with exponential clustering implied by the spectral gap.

Nontrivial bounds on extractable energy in quantum energy teleportation for gapped manybody systems with a unique ground state

TL;DR

This work proves a universal, nonperturbative upper bound on the net energy extractable via Quantum Energy Teleportation (QET) in finite-range gapped lattice systems with a unique ground state: the energy difference between sender and receiver obeys , where is the separation and are set by the spectral gap, interaction range, and local operator norms. The authors combine a variational reduction with exponential clustering (via Lieb-Robinson bounds and the gap) and a careful local-decomposition analysis to bound cross-region correlations, showing that local measurements perturb the ground state only in a finite neighbourhood and that classical communication cannot overcome this to achieve substantial energy transfer at large . A refinement using commutator structure of decoding unitaries yields potentially tighter prefactors when has a local generator. The results provide rigorous justification for the locality of QET effects and offer a route to compute explicit constants for specific models, with potential extensions to thermal states and more general quantum operations.

Abstract

We establish a universal, exponentially decaying upper bound on the average energy that can be extracted in quantum energy teleportation (QET) protocols executed on finite-range gapped lattice systems possessing a unique ground state. Under mild regularity assumptions on the Hamiltonian and uniform operator-norm bounds on the local measurement operators, there exist positive constants and (determined by the spectral gap, interaction range and local operator norms) such that for any local measurement performed in a region and any outcome-dependent local unitaries implemented in a disjoint region separated by distance one has The bound is nonperturbative, explicit up to model-dependent constants, and follows from the variational characterization of the ground state combined with exponential clustering implied by the spectral gap.
Paper Structure (9 sections, 1 theorem, 27 equations)

This paper contains 9 sections, 1 theorem, 27 equations.

Key Result

Lemma 4.1

Let $H$ be a finite-range Hamiltonian with a unique ground state $\omega$ and spectral gap $\Delta>0$. There exist constants $c,\xi>0$ (depending on $\Delta$, $J$, and $r$) such that for any bounded operators $O_Y$ supported on $Y$ and $O_Z$ supported on $Z$,

Theorems & Definitions (1)

  • Lemma 4.1: Exponential clustering