Theories with no superluminal signaling have greater information-processing power than theories with no superluminal causation
Pith reviewed 2026-05-24 04:00 UTC · model grok-4.3
The pith
Theories with no superluminal causation cannot achieve certain correlation tasks that no-superluminal-signaling theories can.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
There exists a spacetime configuration in which the task of generating non-classical correlations cannot be achieved in any theory satisfying no superluminal causation, but theories violating no superluminal causation while satisfying no superluminal signaling can perfectly achieve the task. A protocol is provided for operational certification in general spacetimes, and in (1+1)D Minkowski spacetime the task remains achievable even when measurement outcomes occur arbitrarily earlier than the settings.
What carries the argument
The formal distinction between no superluminal causation (NSC) and no superluminal signaling (NSS) applied to a correlation generation task in a specific spacetime configuration.
Load-bearing premise
The definitions of NSC and NSS as distinct, and the selected spacetime configuration and task, accurately isolate the difference in processing power without extra modeling assumptions.
What would settle it
A concrete counterexample would be any theory satisfying NSC that nonetheless succeeds at the task in the described spacetime configuration.
Figures
read the original abstract
A central goal in the foundations of physics is to understand the structure of physical theories, such as quantum theory, from physical principles. This is often explored by considering various information-theoretic principles. Here, we initiate a similar approach considering relativistic causality principles. No superluminal causation (NSC) and no superluminal signalling (NSS) are distinct relativistic principles, requiring, respectively, that causal influence/the ability of agents to signal are within the future lightcone. After formalizing their distinction, we investigate how well theories constrained by NSC and NSS perform in a task that involves generating non-classical correlations. We find a spacetime configuration in which this task cannot be achieved in any theory (classical, quantum, or post-quantum) satisfying NSC. However, we show that theories violating NSC but satisfying NSS can perfectly achieve the task. We give a protocol that would, in a world allowing superluminal causation, enable its operational certification without violating NSS, in general spacetimes. In the case of $(1+1)$D Minkowski spacetime, the task remains achievable in a configuration where measurement outcomes occur arbitrarily earlier in time than the settings, allowing a new form of certifiable retrocausality without violating NSS. We illustrate our results by linking two different types of non-classical post-quantum resources: PR-boxes and jamming. Our work offers insights into the role of different relativistic causality principles in fundamental physics and paves the way for characterising the information-theoretic structure of theories obeying such principles.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript formalizes the distinction between no superluminal causation (NSC) and no superluminal signalling (NSS) as relativistic principles. It identifies a spacetime configuration and task for generating non-classical correlations that cannot be achieved in any theory (classical, quantum, or post-quantum) satisfying NSC, but can be perfectly achieved in theories violating NSC while satisfying NSS. It supplies an explicit protocol for operational certification of the task in general spacetimes, including a (1+1)D Minkowski case enabling certifiable retrocausality without NSS violation, and illustrates the separation via PR-boxes and jamming resources.
Significance. If the central separation holds, the result demonstrates that NSS permits strictly greater information-processing power than NSC by enabling an otherwise impossible task. The explicit operational definitions in §2, the impossibility argument for NSC theories, and the constructive protocol in §4 constitute clear strengths, as does the direct derivation of the retrocausality example from the same definitions without additional modeling assumptions.
minor comments (2)
- [§2] §2: the operational distinction between NSC and NSS would be easier to track if the definitions were accompanied by a short side-by-side comparison of the allowed causal influences and signalling capabilities.
- [§4] §4: the protocol description would benefit from an explicit spacetime diagram (with labeled agent world-lines, measurement events, and light cones) to make the configuration and the retrocausality claim visually immediate.
Simulated Author's Rebuttal
We thank the referee for their positive summary, recognition of the manuscript's strengths, and recommendation of minor revision. No major comments are provided in the report.
Circularity Check
No significant circularity detected
full rationale
The paper's derivation is self-contained: section 2 supplies independent operational definitions of NSC and NSS that do not presuppose the target separation; the impossibility result for NSC theories follows directly from those definitions applied to the chosen spacetime configuration and task; the explicit protocol in section 4 realizes the task under NSS without invoking fitted parameters, self-referential equations, or load-bearing self-citations. The (1+1)D retrocausality example is likewise obtained by direct substitution of the same definitions. No step reduces by construction to its inputs, and the central claim therefore rests on logically independent content rather than circular reduction.
Axiom & Free-Parameter Ledger
axioms (1)
- standard math Spacetime causal structure is defined by light cones in Minkowski geometry
invented entities (1)
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The specific task requiring non-classical correlations under chosen spacetime configuration
no independent evidence
Lean theorems connected to this paper
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IndisputableMonolith/Foundation/AlexanderDuality.leanalexander_duality_circle_linking unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
Theorem 2. Tasks 1 and 2 can both be achieved in a classical theory that allows for jamming, without violating NSS... Protocol 1... B = A.C... B = X ⊕ Z
What do these tags mean?
- matches
- The paper's claim is directly supported by a theorem in the formal canon.
- supports
- The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
- extends
- The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
- uses
- The paper appears to rely on the theorem as machinery.
- contradicts
- The paper's claim conflicts with a theorem or certificate in the canon.
- unclear
- Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.
Forward citations
Cited by 1 Pith paper
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Characterizing Signalling: Connections between Causal Inference and Space-time Geometry
Introduces the order-theoretic property of conicality for space-times and proves a correspondence between conical space-times and faithful information-theoretic causal models under no-superluminal-signalling constraints.
Reference graph
Works this paper leans on
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[1]
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work page 1996
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[2]
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[3]
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work page 2022
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[4]
Vilasini, V. & Colbeck, R. Impossibility of superluminal signaling in Minkowski spacetime does not rule out causal loops. Physical Review Letters 129, 110401 (2022). link
work page 2022
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[5]
Vilasini, V. & Colbeck, R. A causal modelling analysis of bell scenarios in space-time: implications of jamming non-local correlations for relativistic causality principles (2023). link, 2311.18465
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Causality: Models, reasoning, and inference
Pearl, J. Causality: Models, reasoning, and inference. Second edition, Cambridge University Press (2009). link
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Barrett, J., Lorenz, R. & Oreshkov, O. Quantum causal models. arXiv:1906.10726 (2020). link
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Bell, J. S. Speakable and unspeakable in quantum me- chanics. Cambridge University Press (1987)
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Wood, C. J. & Spekkens, R. W. The lesson of causal discovery algorithms for quantum correlations: causal explanations of Bell-inequality violations require fine- tuning. New Journal of Physics 17, 033002 (2015). link
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[11]
Wiseman, H. M. & Cavalcanti, E. G. Causarum in- vestigatio and the two Bell’s theorems of John Bell. arXiv:1503.06413 (2015). link. 5 A FURTHER DETAILS OF THE CAUSAL MODELLING FRAMEWORK Appendix A: Further details of the causal modelling framework In the main text, we have provided a rather non- technical overview of the causality framework of [3, 4] whic...
work page internal anchor Pith review Pith/arXiv arXiv 2015
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[12]
Hence, (Λ ⊥d AC), which implies the conditional independence P (Λ|AC) = P (Λ)
Since Λ is not embedded in the space-time future of A or C, and A and C have no incoming arrows in the causal model, using NSC it follows that all paths between Λ and AC must contain a collider. Hence, (Λ ⊥d AC), which implies the conditional independence P (Λ|AC) = P (Λ)
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[13]
Since X and Z are spacelike separated, NSC means there are no directed paths between X and Z in the causal model. There could be a collider where the central variable W is embedded in the future of both X and Z, or a fork where the central variable is embedded in the past of X and Z. Candidates for the central variable in a fork are Λ or a vari- able unde...
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[14]
Since X and C are spacelike separated, NSC means there are no directed paths between X and C in the causal model. Since C has no incoming ar- rows, all paths between X and C must contain a collider with central variable in the future of C. It follows that ( X ⊥d C|AΛ), and conse- quently P (X|ΛAC) = P (X|ΛA). Symmetrically, we also have (Z ⊥d A|CΛ) and he...
discussion (0)
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