Teleparallel Palatini theories

被引:193
作者
Beltran Jimenez, Jose [1 ,2 ]
Heisenberg, Lavinia [3 ]
Koivisto, Tomi S. [4 ,5 ,6 ,7 ]
机构
[1] Univ Autonoma Madrid, CSIC, Inst Fis Teor, E-28049 Madrid, Spain
[2] Univ Salamanca, Dept Fis Fundamental, Plaza Merced, E-37008 Salamanca, Spain
[3] Swiss Fed Inst Technol, Inst Theoret Studies, Clausiusstr 47, CH-8092 Zurich, Switzerland
[4] KTH Royal Inst Technol, Nordita, Roslagstullsbacken 23, S-10691 Stockholm, Sweden
[5] Stockholm Univ, Roslagstullsbacken 23, S-10691 Stockholm, Sweden
[6] Helsinki Inst Phys, POB 64, FIN-00014 Helsinki, Finland
[7] Univ Helsinki, Dept Phys Sci, POB 64, FIN-00014 Helsinki, Finland
来源
JOURNAL OF COSMOLOGY AND ASTROPARTICLE PHYSICS | 2018年 / 08期
关键词
gravity; modified gravity; GENERAL-RELATIVITY; ENERGY-MOMENTUM; FIELD-EQUATIONS; NOETHER CHARGE; GRAVITY; TENSOR; FORMULATION; INTEGRALS; ENTROPY; SPIN;
D O I
10.1088/1475-7516/2018/08/039
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
The Palatini formalism, which assumes the metric and the affine connection as independent variables, is developed for gravitational theories in flat geometries. We focus on two particularly interesting scenarios. First, we fix the connection to be metric compatible, as done in the usual teleparallel theories, but we follow a completely covariant approach by imposing the constraints with suitable Lagrange multipliers. For a general quadratic theory we show how torsion naturally propagates and we reproduce the Teleparallel Equivalent of General Relativity as a particular quadratic action that features an additional Lorentz symmetry. We then study the much less explored theories formulated in a geometry with neither curvature nor torsion, so that all the geometrical information is encoded in the non-metricity. We discuss how this geometrical framework leads to a purely inertial connection that can thus be completely removed by a coordinate gauge choice, the coincident gauge. From the quadratic theory we recover a simpler formulation of General Relativity in the form of the Einstein action, which enjoys an enhanced symmetry that reduces to a second linearised diffeomorphism at linear order. More general theories in both geometries can be formulated consistently by taking into account the inertial connection and the associated additional degrees of freedom. As immediate applications, the new cosmological equations and their Newtonian limit are considered, where the role of the lapse in the consistency of the equations is clarified, and the Schwarzschild black hole entropy is computed by evaluating the corresponding Euclidean action. We discuss how the boundary terms in the usual formulation of General Relativity are related to different choices of coordinates in its coincident version and show that in isotropic coordinates the Euclidean action is finite without the need to introduce boundary or normalisation terms. Finally, we discuss the double-copy structure of the gravity amplitudes and the bootstrapping of gravity within the framework of coincident General Relativity.
引用
收藏
页数:48
相关论文
共 116 条
  • [1] Adak M, 2005, TURK J PHYS, V29, P1
  • [2] Lagrange formulation of the symmetric teleparallel gravity
    Adak, Muzaffer
    Kalay, Mestan
    Sert, Ozcan
    [J]. INTERNATIONAL JOURNAL OF MODERN PHYSICS D, 2006, 15 (05): : 619 - 634
  • [3] Adak M, 2006, TURK J PHYS, V30, P379
  • [4] SYMMETRIC TELEPARALLEL GRAVITY: SOME EXACT SOLUTIONS AND SPINOR COUPLINGS
    Adak, Muzaffer
    Sert, Ozcan
    Kalay, Mestan
    Sari, Murat
    [J]. INTERNATIONAL JOURNAL OF MODERN PHYSICS A, 2013, 28 (32):
  • [5] Aldrovandi R., 2013, FUND THEOR PHYS, V173
  • [6] Generalized Proca action for an Abelian vector field
    Allys, Erwan
    Peter, Patrick
    Rodriguez, Yeinzon
    [J]. JOURNAL OF COSMOLOGY AND ASTROPARTICLE PHYSICS, 2016, (02):
  • [7] Unifying Einstein and Palatini gravities
    Amendola, Luca
    Enqvist, Kari
    Koivisto, Tomi
    [J]. PHYSICAL REVIEW D, 2011, 83 (04):
  • [8] [Anonymous], 2004, P 17 INT C GR17 DUBL
  • [9] [Anonymous], ARXIV170501072
  • [10] [Anonymous], 2007, HDB PHILOS SCI PHILO