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.
Status matrix
Section titled “Status matrix”| Statement | Mathematical status in stated domain | Main hypotheses | Equality or saturation | Stability question | Known route to failure outside domain |
|---|---|---|---|---|---|
| Passivity | Structural theorem for declared cyclic operations | Dynamics, energy domain, passive state | Ground/KMS examples; operation-dependent equality | Restrict or enlarge local operation algebra | Omit controller work or allow a forbidden collective operation |
| Complete passivity KMS/ground structure | Structural theorem under -dynamical assumptions | Every finite tensor power, common dynamics | Equilibrium state on every copy number | Catalysts, charges, infinite-energy limits | Test only product unitaries or change composition rules |
| Free-field timelike QEI | Rigorous field- and sampler-specific lower bounds | Renormalized stress tensor, smooth sampler, state class | Optimized states or limiting sequences in special cases | Mass, curvature, boundary, interaction | Take a pointwise limit without scaling the bound |
| ANEC | Proven in broad but hypothesis-dependent relativistic QFT settings | Complete affine null line, convergence, unitarity/causality or modular assumptions | State- and theory-dependent | Defects, boundaries, noncomplete generators | Use a finite null segment |
| Regional relative-entropy bound | Exact positivity identity | Same region, state pair, known modular Hamiltonian | First-order perturbations saturate the first law | Reference, region, species, algebra | Replace weighted modular energy by unweighted total energy |
| QNEC | General continuum proofs under stated smoothness and renormalization assumptions | Null shape variation, renormalized , compatible normalization | Vacuum and special states can saturate | Defects, nonsmooth cuts, gauge-algebra choices | Retain regulator motion in |
| Quantum interest | Derived in specified models from QEIs | Smooth pulse profiles and full energy history | Optimized profiles or limiting configurations | Interaction, boundary, sampling class | Use delta pulses or omit late positive tails |
| Absolute entropy bound at fixed cutoff | Regulator-dependent statement, not universal QFT theorem | Species, cutoff, factorization convention | Scheme dependent | Large species number and limit order | Change or at fixed long-distance state |
| Landauer cost | Exact relative-entropy balance with ideal and finite-reservoir refinements | Memory, bath, reset error, full cycle | Quasistatic infinite-bath limit | Finite time, reservoir depletion, charges | Consume bath athermality or omit record reset |
| Quantum energy teleportation | Valid finite-model protocol; continuum and experimental scope model specific | Correlated state, local instrument, causal message, conditional operation | Model-dependent optimization | Noise, separation, local passivity, continuum limit | Remove 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.
How the statements connect
Section titled “How the statements connect”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.
Falsification sequence
Section titled “Falsification sequence”For any proposed new bound:
- state the spacetime, field, state and operator domain;
- write the precise sampling, region, or shape derivative;
- freeze the regulator, species and charge sector;
- declare the allowed instrument and causal feed-forward;
- account separately for injected, extracted, switching and reset energy;
- reproduce a saturating case and a known outside-domain counterexample;
- perturb the saturation example and test numerical stability.
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.
Interpretation of evidence
Section titled “Interpretation of evidence”“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.
References
Section titled “References”- 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.