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Energy–Information Bounds: Assumptions and Status

Energy–information claims can be compared only after their mathematical inputs and evidence classes are separated. The matrix below records theorem domain, saturation mechanism, model evidence, and characteristic counterexample. It reflects literature available through 10 August 2026 and should be read together with the detailed pages.

Required background. Review passivity, QEIs, ANEC, relative-entropy bounds, QNEC, quantum interest, species and regulators, Landauer erasure, and QET before using this comparison.

StatementMathematical status in stated domainMain hypothesesEquality or saturationStability questionKnown route to failure outside domain
PassivityStructural theorem for declared cyclic operationsDynamics, energy domain, passive stateGround/KMS examples; operation-dependent equalityRestrict or enlarge local operation algebraOmit controller work or allow a forbidden collective operation
Complete passivity \Leftrightarrow KMS/ground structureStructural theorem under CC^*-dynamical assumptionsEvery finite tensor power, common dynamicsEquilibrium state on every copy numberCatalysts, charges, infinite-energy limitsTest only product unitaries or change composition rules
Free-field timelike QEIRigorous field- and sampler-specific lower boundsRenormalized stress tensor, smooth sampler, state classOptimized states or limiting sequences in special casesMass, curvature, boundary, interactionTake a pointwise limit without scaling the bound
ANECProven in broad but hypothesis-dependent relativistic QFT settingsComplete affine null line, convergence, unitarity/causality or modular assumptionsState- and theory-dependentDefects, boundaries, noncomplete generatorsUse a finite null segment
Regional relative-entropy boundExact positivity identitySame region, state pair, known modular HamiltonianFirst-order perturbations saturate the first lawReference, region, species, algebraReplace weighted modular energy by unweighted total energy
QNECGeneral continuum proofs under stated smoothness and renormalization assumptionsNull shape variation, renormalized TkkT_{kk}, compatible normalizationVacuum and special states can saturateDefects, nonsmooth cuts, gauge-algebra choicesRetain regulator motion in SS''
Quantum interestDerived in specified models from QEIsSmooth pulse profiles and full energy historyOptimized profiles or limiting configurationsInteraction, boundary, sampling classUse delta pulses or omit late positive tails
Absolute entropy bound at fixed cutoffRegulator-dependent statement, not universal QFT theoremSpecies, cutoff, factorization conventionScheme dependentLarge species number and limit orderChange NN or ϵ\epsilon at fixed long-distance state
Landauer costExact relative-entropy balance with ideal and finite-reservoir refinementsMemory, bath, reset error, full cycleQuasistatic infinite-bath limitFinite time, reservoir depletion, chargesConsume bath athermality or omit record reset
Quantum energy teleportationValid finite-model protocol; continuum and experimental scope model specificCorrelated state, local instrument, causal message, conditional operationModel-dependent optimizationNoise, separation, local passivity, continuum limitRemove message/correlation or omit injected energy

No row licenses a claim outside its hypothesis column. A counterexample to a heuristic extension does not refute the restricted theorem.

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.

The map groups results by principal input. Connections between branches require additional arguments; no vertical or horizontal position represents theorem strength. The diagram is schematic.

Passivity and Landauer reasoning use equilibrium structure and operation classes; the exact complete-passivity characterization is Pusz and Woronowicz 1978, Theorems 1.1 and 1.4, pp. 275–281. QEIs and ANEC use averaged stress energy, with the sampler and state domains reviewed in Fewster 2012, §§ 2–4, pp. 6–20. Regional bounds and QNEC use modular or entropic data; a general QNEC proof and its assumptions are given by Balakrishnan et al. 2019, §§ 2–5. QET is an operational protocol constrained by, but not equivalent to, any one of these inequalities.

For any proposed new bound:

  1. state the spacetime, field, state and operator domain;
  2. write the precise sampling, region, or shape derivative;
  3. freeze the regulator, species and charge sector;
  4. declare the allowed instrument and causal feed-forward;
  5. account separately for injected, extracted, switching and reset energy;
  6. reproduce a saturating case and a known outside-domain counterexample;
  7. perturb the saturation example and test numerical stability.

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.

Domain, averaging, renormalization, and operational accounting are independent gates. A claim that survives only because one gate was not varied is not stable evidence for a new bound. The map is schematic.

“Proven” means a theorem under stated hypotheses, not experimentally realized. “Model-checked” means evaluated in a controlled Hamiltonian or QFT example. “Hardware executed” means a finite encoded protocol ran on a device; it does not by itself validate a continuum limit. “Conjectural” should identify both the unproved statement and known restricted results. A result can be rigorous, saturable, and still too narrow for a proposed application.

  • Balakrishnan, Souvik, Thomas Faulkner, Zuhair U. Khandker, and Huajia Wang. “A General Proof of the Quantum Null Energy Condition.” Journal of High Energy Physics 2019, no. 9 (2019): 020. DOI.
  • Fewster, Christopher J. “Lectures on Quantum Energy Inequalities.” In Quantum Field Theory and Gravity, edited by Felix Finster et al., 2012. arXiv.
  • Pusz, Władysław, and Stanisław L. Woronowicz. “Passive States and KMS States for General Quantum Systems.” Communications in Mathematical Physics 58 (1978): 273–290. DOI.