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How to detect the spacetime curvature without rulers and clocks. II. Three-dimensional spacetime

2023/12/06 by A. V. Nenashev, Nenashev, A. V., S. D. Baranovskiǐ +1
Mathematics · Medicine · Physics and Astronomy · #Biofield Effects and Biophysics #Causal sets #Causal structure #Curvature #Differential Geometry (math.DG) #FOS: Mathematics #FOS: Physical sciences #General Relativity and Quantum Cosmology (gr-qc) #General relativity #Geometry #Mathematical physics #Mathematics #Mathematics of general relativity #Maxwell's equations in curved spacetime #Metric (unit) #Minkowski space #Numerical relativity #Physics #Quantum field theory in curved spacetime #Quantum gravity #Quantum mechanics #Radioactive Decay and Measurement Techniques #Relativity and Gravitational Theory #Spacetime #Spacetime symmetries #Spacetime topology #Spherically symmetric spacetime #Stationary spacetime #Theoretical physics #World line

paper · pdf · doi:10.48550/arxiv.2312.03487

published in arXiv (Cornell University) (Cornell University)

openalex publication_date 2023/12/06 · openalex created_date 2023/12/08 · openalex updated_date 2026/07/28

Abstract

We have generalized the results of the previous work [arXiv:2302.12209] to the case of three-dimensional (3D) spacetime with two spatial and one temporal coordinates. We have found that the flat Minkowski 3D spacetime is "well-stitched", which means that it possesses a structure described by 24 causal relations between 12 events. We have proved that a 3D spacetime is "well-stitched" if and only if it is conformally flat. The concept of a "well-stitched" spacetime does not rely on metrical information about lengths, times, etc., and does not belong to the metric geometry, but rather to geometry of incidence. We therefore have "translated" an important concept of a conformally-flat spacetime from the "metric" language of Riemannian geometry to the "non-metric" language of the geometry of incidence. The results of this paper provide a tool for detecting the curvature of the 3D spacetime on the basis of causal relations only, without any measurement instruments like rulers and clocks, provided that the spacetime is not conformally flat.

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