2023/11/09 by Hans Oude Groeniger, Groeniger, Hans Oude
Physics and Astronomy · #83C20 #83C75 #83F05 #Advanced Differential Geometry Research #Black Holes and Theoretical Physics #Cosmology and Gravitation Theories #FOS: Physical sciences #General Relativity and Quantum Cosmology (gr-qc) #Mathematical Physics (math-ph)
paper · pdf · doi:10.48550/arxiv.2311.05522
openalex publication_date 2023/11/09 · openalex created_date 2025/10/10 · openalex updated_date 2026/07/28
Cosmologies of the lower Bianchi types, i.e. except those of type VIII or IX, admit a two-dimensional Abelian subgroup of the isometry group, the G2. In orthogonal perfect fluid cosmologies of all lower Bianchi types except for type VI-1/9 the G2 acts orthogonally-transitively, which is closely related to an eventual cessation of the oscillations and thus to a quiescent singularity. But due to a degeneracy in the momentum constraints, such cosmologies of type VI-1/9 do not necessarily have this property. As a consequence, the dynamics of type VI-1/9 orthogonal perfect fluid cosmologies have the same degrees of freedom as those of the higher types VIII and IX and their dynamics are expected to be markedly different compared to those of the other lower Bianchi types. In this article we take a different approach to quiescence, namely the presence of an orthogonal stiff fluid. On the one hand, this completes the analysis of the initial singularity for all Bianchi orthogonal stiff fluid cosmologies. On the other hand, this allows us to get a grasp of the underlying dynamics of type VI-1/9 perfect fluid cosmologies, in particular the effect of orthogonal transitivity as well as possible (asymptotic) polarization conditions. In particular, we show that a generic type VI-1/9 cosmology with an orthogonal stiff fluid has similar asymptotics as a generic Bianchi type VIII or IX cosmology with an orthogonal stiff fluid. The only exceptions to this genericity are solutions satisfying (asymptotic) polarization conditions, and solutions for which the G2 acts orthogonally-transitively. Only in those cases may the limits of the eigenvalues of the expansion-normalized Weingarten map be negative.