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This study establishes a fundamental no-go theorem proving that classical massless particles, such as photons or gravitons, cannot emerge from the coarse-grained limit of quantum fields while maintaining relativistic covariance. The authors demonstrate through an axiomatic kinematical framework that field-like limits remain viable for phenomena like electromagnetism and gravity, but discrete particle descriptions are mathematically incompatible with operational classicality in this regime.
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No classical particle limit for massless quanta

arXiv2 min de cititArticolul și perspectiva sunt în engleză.

arXiv:2606.14632v1 Announce Type: new Abstract: We investigate whether relativistic massless classical particles may emerge as the classical limit of massless quanta. To address this question independently of any specific dynamics, environment, or pointer basis, we develop an axiomatic and purely kinematical framework for the coarse-graining approach. In this formulation, a candidate classical phase space is taken as the outcome space of a POVM subject only to minimal classicality and covariance under the relevant spacetime symmetry group. Applying this framework to the Poincar\'e group, we prove a no-go theorem for massless particles: the covariance requirement is incompatible with the operational conditions for classicality. The theorem leaves open field-like limits of massless quanta, for example the emergence of electromagnetic or gravitational fields, while ruling out classical massless particles, such as classical photons or gravitons.

Abstract:We investigate whether relativistic massless classical particles may emerge as the classical limit of massless quanta. To address this question independently of any specific dynamics, environment, or pointer basis, we develop an axiomatic and purely kinematical framework for the coarse-graining approach. In this formulation, a candidate classical phase space is taken as the outcome space of a POVM subject only to minimal classicality and covariance under the relevant spacetime symmetry group. Applying this framework to the Poincaré group, we prove a no-go theorem for massless particles: the covariance requirement is incompatible with the operational conditions for classicality. The theorem leaves open field-like limits of massless quanta, for example the emergence of electromagnetic or gravitational fields, while ruling out classical massless particles, such as classical photons or gravitons.

arXiv:2606.14632 [quant-ph]

(or arXiv:2606.14632v1 [quant-ph] for this version)

https://doi.org/10.48550/arXiv.2606.14632 Focus to learn more arXiv-issued DOI via DataCite (pending registration)

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