Azimuthal geodesics in closed FLRW cosmologies

Fuente: arXiv
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Autores principales: Boehmer, Christian G., del Sordo, Antonio d'Alfonso, Hartmann, Betti
Formato: Preprint
Publicado: 2024
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author Boehmer, Christian G.
del Sordo, Antonio d'Alfonso
Hartmann, Betti
author_facet Boehmer, Christian G.
del Sordo, Antonio d'Alfonso
Hartmann, Betti
contents Modern cosmology is closely linked to our understanding of radial null geodesics as these model the propagation of light signals through an expanding universe. Azimuthal geodesics, on the other hand, are perhaps best known for their relevance within closed cosmological models. Such models typically have a finite lifetime: the universe expands up to a maximum size after which it recollapses during the so-called big crunch. An azimuthal geodesic starting at the beginning of the universe will travel a finite angular distance during the expansion and recollapse. It is well-known that this angle is $2π$ for a matter-dominated universe and $π$ for a radiation-dominated solution. Here we derive the simple formula $$Δφ= \frac{2π}{1+3w}$$ for an arbitrary linear equation of state parameter $w$. To the best of our knowledge this result has not been reported elsewhere and fills a small gap in the literature.
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institution arXiv
publishDate 2024
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spellingShingle Azimuthal geodesics in closed FLRW cosmologies
Boehmer, Christian G.
del Sordo, Antonio d'Alfonso
Hartmann, Betti
General Relativity and Quantum Cosmology
Modern cosmology is closely linked to our understanding of radial null geodesics as these model the propagation of light signals through an expanding universe. Azimuthal geodesics, on the other hand, are perhaps best known for their relevance within closed cosmological models. Such models typically have a finite lifetime: the universe expands up to a maximum size after which it recollapses during the so-called big crunch. An azimuthal geodesic starting at the beginning of the universe will travel a finite angular distance during the expansion and recollapse. It is well-known that this angle is $2π$ for a matter-dominated universe and $π$ for a radiation-dominated solution. Here we derive the simple formula $$Δφ= \frac{2π}{1+3w}$$ for an arbitrary linear equation of state parameter $w$. To the best of our knowledge this result has not been reported elsewhere and fills a small gap in the literature.
title Azimuthal geodesics in closed FLRW cosmologies
topic General Relativity and Quantum Cosmology
url https://arxiv.org/abs/2401.04597