The scalar-tensor theory of gravitation

By 藤井保憲, 前田恵一. 2003

254 citations recorded by the source corpus.

View Paper: https://www.semanticscholar.org/paper/af8ac563785c06b2c3596d61ec7ed0554e358367

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Citations in the corpus

Black holes, gravitational waves and fundamental physics: a roadmap (2018, background): “Prominent exceptions are (single- or multi-) scalar-tensor (ST) theories of gravity [1198] which includes Brans-Dicke theory [1199] and, through mathematical equivalence, a subset of f(R) theories [1200]. ST theories inherit the well-posedness of GR through the Einstein frame formulation [1201]; see”
Cosmology and brane worlds: a review (2003, background): “As such it has much in common with scalar–tensor theories [90], but there are important differences due to the projected Weyl tensor Eμν and its time–evolution.”
Crossing of the phantom divide in modified gravity (2008, methodology): “Consequently, the action in the Einstein frame is given by [39, 48] SE = ∫”
f(R) Theories (2010, methodology): “It is possible to derive an action in the Einstein frame under the conformal transformation [213, 609, 408, 611, 249, 268, 410]: gμν = Ω 2 gμν , (2.”
Gravitational radiation from compact binary systems in the massive Brans-Dicke theory of gravity (2011, methodology): “Now let us make the conformal transformation gμν → ψ(2)(φ)gμν , and in doing so move into a conformal frame in which the matter fields do not couple directly (but only indirectly, via the metric) to the scalar field; this is commonly referred to as the Jordan frame [1, 3].”
Inflation and late-time cosmic acceleration in non-minimal Maxwell-F(R) gravity and the generation of large-scale magnetic fields (2008, background): “Consequently, the action in the new conformal frame is given by [50] SN = ∫”
Black hole based tests of general relativity (2016, background): “The first example that we consider is scalar-tensor theories [162].”