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Bell Factorization, Trace-Class Conditions, and Functional Fine-Tuning: A Dictionary between Quantum Field Theory and Classical Causal Models

Eduardo Gonzalez-Granda Fernandez

Published Apr 27, 2026• 0 citations
Publisher

Abstract

This work develops a functional-analytic dictionary between Bell-type factorizations and correlation kernels in relativistic quantum field theory (QFT). We show that uniformly bounded Bell factorizations correspond to finite local trace conditions on quadratic forms, while divergence of the trace forces any approximating factorization to exhibit unbounded L² norms. This provides a precise functional interpretation of fine-tuning in classical causal models, identifying it with instability under approximation. The results establish a bridge between three frameworks: (i) hidden-variable factorizations, (ii) quadratic forms on test functions, and (iii) structural properties of QFT correlation functions. In particular, typical short-distance singularities suggest that infinite trace — and therefore functional fine-tuning — is generic in QFT. This paper serves as a conceptual dictionary linking previous results on trace-class obstructions with causal-model interpretations of quantum correlations.

DOI
10.5281/zenodo.19817251

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This work develops a functional-analytic dictionary between Bell-type factorizations and correlation kernels in relativistic quantum field theory (QFT). We show that uniformly bounded Bell factorizations correspond to finite local trace conditions on quadratic forms, while divergence of the trace forces any approximating factorization to exhibit unbounded L² norms. This provides a precise functional interpretation of fine-tuning in classical causal models, identifying it with instability under approximation. The results establish a bridge between three frameworks: (i) hidden-variable factorizations, (ii) quadratic forms on test functions, and (iii) structural properties of QFT correlation functions. In particular, typical short-distance singularities suggest that infinite trace — and therefore functional fine-tuning — is generic in QFT. This paper serves as a conceptual dictionary linking previous results on trace-class obstructions with causal-model interpretations of quantum correlations.
We establish a functional-analytic obstruction to Bell-type factorizations of two-point distributions in relativisticquantum field theory. Working purely at the level of quadratic forms on test functions, we show that any positive sesquilinear form whoselocal trace diverges cannot admit a Bell factorization with uniformly L²-bounded response functions. Moreover, anyapproximating sequence of such factorizations necessarily exhibits unbounded L² norms — a continuous analogue of theexact cancellations characteristic of fine-tuning in classical causal models. The argument is fully rigorous and self-contained: it uses only finite orthonormal families, Bessel's inequality, andTonelli's theorem, avoiding any need for operator domains or spectral theory. As a physical motivation, we discusshow short-distance singularities in Wightman two-point functions heuristically imply infinite local trace, makingthe obstruction physically relevant. We also provide an explicit spectral computation for the free scalar fieldin four dimensions. The result provides a functional-analytic mechanism underlying Cavalcanti's theorem on fine-tuning in classicalcausal models, and complements our previous spectral no-go theorems for causally localized jamming in QFT. This paper belongs to a series on analytic obstructions to causal factorization in relativistic quantum field theory.
We establish a structural obstruction to bounded Bell-type factorizations of two-point functions in relativistic quantum field theory. Working at the level of bilinear forms on Schwartz space, we show that any Bell-factorizable distribution with uniformly bounded L² response functions satisfies a universal quadratic bound. We then prove that Wightman two-point functions with unbounded spectral density (a standard ultraviolet property in interacting QFT) violate this bound. As a consequence, no such function admits a stable Bell factorization: any approximating sequence of Bell-factorizable distributions necessarily involves response functions whose norms diverge. This provides a functional-analytic formulation of the fine-tuning phenomenon identified by Cavalcanti in causal models, linking spectral properties of quantum field theory to the instability of classical causal representations. The results avoid assumptions of spacetime localization and instead rely solely on spectral structure and positivity, offering a new perspective on the incompatibility between relativistic QFT and classical causal factorizations.
This work investigates structural constraints imposed by analyticity in relativistic quantum field theory on classical causal explanations of quantum correlations. Building on previous results on analytic rigidity, we establish a conditional obstruction to the realization of classical causal factorizations through spacetime-localized modifications of two-point correlation functions. The argument derives analyticity directly from the spectral condition and identifies clustering as the key mechanism linking probabilistic factorization with analytic constraints. We then extend the analysis to three-point functions. A marginal spectral condition is introduced as a natural generalization compatible with dimensional reduction. Under this framework, we prove that any admissible modification must vanish upon reduction to all two-point marginals. The irreducible three-point sector is analyzed via connected correlation functions. A conditional obstruction is obtained under an extended analytic rigidity hypothesis in higher-dimensional tube domains, which is formulated explicitly as an open problem. The work provides a unified perspective connecting analytic properties of quantum field theory with causal modeling approaches to quantum correlations, and outlines a program for extending these results to higher-point functions.
Nonlocality and contextuality are at the root of conceptual puzzles in quantum mechanics, and are key resources for quantum advantage in information-processing tasks. Bell nonlocality is best understood as the incompatibility between quantum correlations and the classical theory of causality, applied to relativistic causal structure. Contextuality, on the other hand, is on a more controversial foundation. In this work, I provide a common conceptual ground between nonlocality and contextuality as violations of classical causality. First, I show that Bell inequalities can be derived solely from the assumptions of no-signalling and no-fine-tuning of the causal model. This removes two extra assumptions from a recent result from Wood and Spekkens, and remarkably, does not require any assumption related to independence of measurement settings -- unlike all other derivations of Bell inequalities. I then introduce a formalism to represent contextuality scenarios within causal models and show that all classical causal models for violations of a Kochen-Specker inequality require fine-tuning. Thus the quantum violation of classical causality goes beyond the case of space-like separated systems, and manifests already in scenarios involving single systems.
In his seminal paper, Bell [Physics Physique Fizika 1, 195 (1964)] considers the correlations that result from space-like separated measurements on a pair of entangled particles. He uses relativity theory to motivate the Bell causal structure, then shows the existence of quantum correlations that cannot be explained classically within this causal structure. Classical explanations of such quantum correlations are possible in alternative causal structures, for instance, those that allow superluminal causal influences, but, as shown in [New Journal of Physics 17 033002 (2015)], all such alternative explanations require fine tuning (causation without correlation). Here we discuss the existence of spurious quantum correlations --- correlations that look quantum in one causal structure, but have a natural classical explanation in another. More precisely, there are causal structures that admit non-classical quantum correlations, but for which the same correlations have a classical explanation in another causal structure without fine tuning. The realisation in the other causal structure can also be achieved without breaking any natural constraints on the causal structure that follow from relativity theory. However, similarly to non-classical quantum correlations in the Bell causal structure, we find other causal structures with non-classical quantum correlations that do not have a classical causal explanation in any alternative causal structure without fine tuning.
This work investigates the compatibility of hidden-variable modifications with the analytic structure of relativistic quantum field theory (QFT). Working within the framework of tempered distributions, we analyze three fundamental properties: the spectral condition, analyticity in the forward tube, and causal localization. We prove a rigidity result showing that any modification satisfying all three conditions must vanish identically. This establishes a structural obstruction linking analyticity and causal constraints in QFT. Building on this result, we provide a systematic classification of nontrivial hidden-variable extensions according to which analytic assumptions fail. We identify three distinct regimes: (i) delocalized modifications compatible with standard QFT, (ii) causally localized modifications that violate the spectral condition and introduce negative-frequency components, and (iii) localized modifications that necessarily break analyticity. These results show that nontrivial hidden-variable theories cannot be embedded within the standard analytic framework of relativistic QFT without violating at least one of its fundamental structural principles. The work provides a unified analytic perspective on the constraints governing hidden-variable extensions and clarifies the role of analyticity as a rigidity mechanism.