scholarly journals Gauge-invariant effective stress-energy tensors for gravitational waves

1997 ◽  
Vol 55 (6) ◽  
pp. 3440-3443 ◽  
Author(s):  
Paul R. Anderson
2003 ◽  
Vol 68 (10) ◽  
Author(s):  
Ioannis Kouletsis ◽  
Petr Hájíček ◽  
Jiří Bičák

2018 ◽  
Vol 15 (03) ◽  
pp. 1850045 ◽  
Author(s):  
Alcides Garat

The relationship between gauge and gravity amounts to understanding the underlying new geometrical local structures. These structures are new tetrads specially devised for Yang–Mills theories, Abelian and non-Abelian in four-dimensional Lorentzian curved spacetimes. In the present paper, a new tetrad is introduced for the Yang–Mills [Formula: see text] formulation. These new tetrads establish a link between local groups of gauge transformations and local groups of spacetime transformations that we previously called LB1 and LB2. New theorems are proved regarding isomorphisms between local internal [Formula: see text] groups and local tensor products of spacetime LB1 and LB2 groups of transformations. These new tetrads define at every point in spacetime two orthogonal planes that we called blades or planes one and two. These are the local planes of covariant diagonalization of the stress–energy tensor. These tetrads are gauge dependent. Tetrad local gauge transformations leave the tetrads inside the local original planes without leaving them. These local tetrad gauge transformations enable the possibility to connect local gauge groups Abelian or non-Abelian with local groups of tetrad transformations. On the local plane one, the Abelian group [Formula: see text] of gauge transformations was already proved to be isomorphic to the tetrad local group of transformations LB1, for example. LB1 is [Formula: see text] plus two different kinds of discrete transformations. On the local orthogonal plane two [Formula: see text] is isomorphic to LB2 which is just [Formula: see text]. That is, we proved that LB1 is isomorphic to [Formula: see text] which is a remarkable result since a noncompact group plus two discrete transformations is isomorphic to a compact group. These new tetrads have displayed manifestly and nontrivially the coupling between Yang–Mills fields and gravity. The new tetrads and the stress–energy tensor allow for the introduction of three new local gauge invariant objects. Using these new gauge invariant objects and in addition a new general local duality transformation, a new algorithm for the gauge invariant diagonalization of the Yang–Mills stress–energy tensor is developed as an application. This is a paper about grand Standard Model gauge theories — General Relativity gravity unification and grand group unification in four-dimensional curved Lorentzian spacetimes.


1986 ◽  
Vol 64 (5) ◽  
pp. 637-640 ◽  
Author(s):  
G. Kunstatter ◽  
D. Vincent

A discussion is given of the Kaluza–Klein monopole and the inherent problem associated with its scalar field. A model that achieves a confinement of this scalar field is presented, whereby a thin boundary layer is imposed on the monopole geometry allowing an exterior geometry with a constant scalar field to be attached. The Gauss–Codazzi formalism then puts strong constraints on the effective stress energy of the boundary.


Universe ◽  
2021 ◽  
Vol 7 (1) ◽  
pp. 9
Author(s):  
Yunqi Liu ◽  
Wei-Liang Qian ◽  
Yungui Gong ◽  
Bin Wang

In this paper, we study the properties of gravitational waves in the scalar–tensor–vector gravity theory. The polarizations of the gravitational waves are investigated by analyzing the relative motion of the test particles. It is found that the interaction between the matter and vector field in the theory leads to two additional transverse polarization modes. By making use of the polarization content, the stress-energy pseudo-tensor is calculated by employing the perturbed equation method. Additionally, the relaxed field equation for the modified gravity in question is derived by using the Landau–Lifshitz formalism suitable to systems with non-negligible self-gravity.


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