Abstract:The quadratic curvature lagrangians having metric field equations with second order trace are constructed relative to an orthonormal coframe. In n > 4 dimensions, pure quadratic curvature lagrangian having second order trace constructed contains three free parameters in the most general case. The fourth order field equations of some of these models, in arbitrary dimensions, are cast in a particular form using the Schouten tensor. As a consequence, the field equations for the New massive gravity theory are rela… Show more
“…The field equations given by Eq. (20) for the CGMG model are valid relative to both an orthonormal coframe [24,25] as well as to the seminull coframe to be defined in the preliminary section above.…”
Section: Field Equations In the Differential Forms Languagementioning
Impulsive, nondiverging, Petrov-Segre type-N gravitational wave solutions to a general massive three-dimensional gravity in the de Sitter, anti-de Sitter and flat Minkowski backgrounds are constructed in a unified manner by using the exterior algebra of differential forms.
“…The field equations given by Eq. (20) for the CGMG model are valid relative to both an orthonormal coframe [24,25] as well as to the seminull coframe to be defined in the preliminary section above.…”
Section: Field Equations In the Differential Forms Languagementioning
Impulsive, nondiverging, Petrov-Segre type-N gravitational wave solutions to a general massive three-dimensional gravity in the de Sitter, anti-de Sitter and flat Minkowski backgrounds are constructed in a unified manner by using the exterior algebra of differential forms.
“…In this section the scheme of calculation of variational derivatives relative to an orthonormal coframe will briefly be presented [29][30][31][32]. In the subsequent sections, the general formulas of this section will be applied to all the modified gravitational actions considered below.…”
Section: Field Equations Relative To An Orthonormal Coframementioning
confidence: 99%
“…The QC Lagrangians having this particular property in arbitrary dimension n ! 3 have been constructed in [31].…”
Section: General Scalar-tensor Equivalence For An Arbitrary Curvamentioning
confidence: 99%
“…However, intending the modification of the quadratic curvature Lagrangian densities in the fðRÞ spirit, it is convenient to work with all three scalars. For further calculational details for the variational derivatives of the Lagrangians relative to an orthonormal coframe considered here, see [30][31][32].…”
A general scheme of constructing scalar-tensor equivalents to modified gravitational actions are studied using the algebra of exterior differential forms and the first order formalism that allows an independent connection and coframe. By introducing appropriate constraints on the connection, pseudo-Riemannian cases as well as non-Riemannian cases are discussed for various gravitational models. The issue of the dynamical degree of freedom for the resulting scalar fields is discussed at the level of the field equations. Explicit scalar-tensor equivalents for gravitational models based on fðRÞ models, the quadratic curvature Lagrangians and the models involving the gradients of the scalar curvature are presented. In particular, explicit scalar-tensor equivalence for gravitational Lagrangians popular in some cosmological models are constructed.
A conserved current for generic quadratic curvature gravitational models is defined and it is shown that at the linearized level it corresponds to the Deser-Tekin charges. An explicit expression for the charge for new massive gravity in three dimensions is given. Some implications of the linearized equations are discussed.
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