On the origin of Poincaré gauge gravity

We argue that the origin of Poincaré gauge gravity (PGG) may be related to spontaneous violation of underlying spacetime symmetries involved and appearance of gauge fields as vector Goldstone bosons. In essence, we start with an arbitrary theory of some vector and fermion fields which possesses only...

Full description

Bibliographic Details
Main Author: J.L. Chkareuli
Format: Article
Language:English
Published: Elsevier 2017-06-01
Series:Physics Letters B
Subjects:
Online Access:http://www.sciencedirect.com/science/article/pii/S0370269317302861
id doaj-5b45a2f5faa44aa6af6409067c104743
record_format Article
spelling doaj-5b45a2f5faa44aa6af6409067c1047432020-11-24T23:05:06ZengElsevierPhysics Letters B0370-26931873-24452017-06-01769C37738410.1016/j.physletb.2017.04.012On the origin of Poincaré gauge gravityJ.L. Chkareuli0Center for Elementary Particle Physics, Ilia State University, 0162 Tbilisi, GeorgiaWe argue that the origin of Poincaré gauge gravity (PGG) may be related to spontaneous violation of underlying spacetime symmetries involved and appearance of gauge fields as vector Goldstone bosons. In essence, we start with an arbitrary theory of some vector and fermion fields which possesses only global spacetime symmetries, such as Lorentz and translational invariance, in flat Minkowski space. The two vector field multiplets involved are assumed to belong, respectively, to the adjoint (Aμij) and vector (eμi) representations of the starting global Lorentz symmetry. We propose that these prototype vector fields are covariantly constrained, AμijAijμ=±MA2 and eμieiμ=±Me2, that causes a spontaneous violation of the accompanying global symmetries (MA,e are their presumed violation scales). It then follows that the only possible theory compatible with these length-preserving constraints is turned out to be the gauge invariant PGG, while the corresponding massless (pseudo)Goldstone modes are naturally collected in the emergent gauge fields of tetrads and spin-connections. In a minimal theory case being linear in a curvature we unavoidably come to the Einstein–Cartan theory. The extended theories with propagating spin-connection and tetrad modes are also considered and their possible unification with the Standard Model is briefly discussed.http://www.sciencedirect.com/science/article/pii/S0370269317302861GravitationAlternative gravity theoriesGauge theoriesSpontaneous symmetry breakingSigma modelsGrand unified models
collection DOAJ
language English
format Article
sources DOAJ
author J.L. Chkareuli
spellingShingle J.L. Chkareuli
On the origin of Poincaré gauge gravity
Physics Letters B
Gravitation
Alternative gravity theories
Gauge theories
Spontaneous symmetry breaking
Sigma models
Grand unified models
author_facet J.L. Chkareuli
author_sort J.L. Chkareuli
title On the origin of Poincaré gauge gravity
title_short On the origin of Poincaré gauge gravity
title_full On the origin of Poincaré gauge gravity
title_fullStr On the origin of Poincaré gauge gravity
title_full_unstemmed On the origin of Poincaré gauge gravity
title_sort on the origin of poincaré gauge gravity
publisher Elsevier
series Physics Letters B
issn 0370-2693
1873-2445
publishDate 2017-06-01
description We argue that the origin of Poincaré gauge gravity (PGG) may be related to spontaneous violation of underlying spacetime symmetries involved and appearance of gauge fields as vector Goldstone bosons. In essence, we start with an arbitrary theory of some vector and fermion fields which possesses only global spacetime symmetries, such as Lorentz and translational invariance, in flat Minkowski space. The two vector field multiplets involved are assumed to belong, respectively, to the adjoint (Aμij) and vector (eμi) representations of the starting global Lorentz symmetry. We propose that these prototype vector fields are covariantly constrained, AμijAijμ=±MA2 and eμieiμ=±Me2, that causes a spontaneous violation of the accompanying global symmetries (MA,e are their presumed violation scales). It then follows that the only possible theory compatible with these length-preserving constraints is turned out to be the gauge invariant PGG, while the corresponding massless (pseudo)Goldstone modes are naturally collected in the emergent gauge fields of tetrads and spin-connections. In a minimal theory case being linear in a curvature we unavoidably come to the Einstein–Cartan theory. The extended theories with propagating spin-connection and tetrad modes are also considered and their possible unification with the Standard Model is briefly discussed.
topic Gravitation
Alternative gravity theories
Gauge theories
Spontaneous symmetry breaking
Sigma models
Grand unified models
url http://www.sciencedirect.com/science/article/pii/S0370269317302861
work_keys_str_mv AT jlchkareuli ontheoriginofpoincaregaugegravity
_version_ 1725627494541819904