Conformal Galilean-type algebras, massless particles and gravitation
Peter C. Stichel

TL;DR
This paper explores conformal Galilean-type algebras and introduces massless particles within these frameworks, demonstrating their potential role in modeling dark energy and cosmic acceleration through self-gravitating systems.
Contribution
It defines conformal Galilean-type algebras for any dynamical exponent and constructs massless particle realizations, linking these to gravitational effects and cosmological phenomena.
Findings
Massless particles exhibit arbitrary finite velocities in these algebras.
Self-gravitating systems with these particles show variable gravitational mass density.
Cosmological models based on these systems display early deceleration and late acceleration phases.
Abstract
After defining conformal Galilean-type algebras for arbitrary dynamical exponent we consider the particular cases of the conformal Galilei algebra (CGA) and the Schr\"odinger Lie algebra (sch). Galilei massless particles moving with arbitrary, finite velocity are introduced \begin{description} \item{i)} in as a realization of the centrally extended CGA in 6 dimensional phase space, \item{ii)} in arbitrary spatial dimension as a realization of the unextended \it{sch} in 4d dimensional phase space. \end{description} A particle system, minimally coupled to gravity, shows, besides Galilei symmetry, also invariance with respect to arbitrary time dependent translations and to dilations with . The most important physical property of such a self-gravitating system is the appearance of a dynamically generated gravitational mass density of either sign. Therefore, this…
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Taxonomy
TopicsCosmology and Gravitation Theories · Relativity and Gravitational Theory · Black Holes and Theoretical Physics
