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General teleparallel quadratic gravity

Jose Beltrán JiménezDepartamento de Física Fundamental and IUFFyM, Universidad de Salamanca, E-37008 Salamanca, SpainLavinia HeisenbergInstitute for Theoretical Physics, ETH Zurich, Wolfgang-Pauli-Strasse 27, 8093, Zurich, SwitzerlandDamianos IosifidisInstitute of Theoretical Physics, Department of Physics, Aristotle University of Thessaloniki, 54124 Thessaloniki, GreeceAlejandro Jiménez-CanoDepartamento de Física Teórica y del Cosmos and CAFPE, Facultad de Ciencias, Avda Fuentenueva s/n, Universidad de Granada, 18071 Granada, SpainTomi KoivistoLaboratory of Theoretical Physics, Institute of Physics, University of Tartu, W. Ostwaldi 1, 50411 Tartu, Estonia
2020en
ABI

Аннотация

In this Letter we consider a general quadratic parity-preserving theory for a general flat connection. Imposing a local symmetry under the general linear group singles out the general teleparallel equivalent of General Relativity carrying both torsion and non-metricity. We provide a detailed discussion on the teleparallel equivalents of General Relativity and how the two known equivalents, formulated on Weitzenböck and symmetric teleparallel geometries respectively, can be interpreted as two gauge-fixed versions of the general teleparallel equivalent. We then explore the viability of the general quadratic theory by studying the spectrum around Minkowski. The linear theory generally contains two symmetric rank-2 fields plus a 2-form and, consequently, extra gauge symmetries are required to obtain potentially viable theories.

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