Motivated by an inclination for symmetry and possible extension of the General Theory of Relativity within the framework of Scalar Theory, we investigate the Bekenstein's disformal transformation of the Einstein-Hilbert action. Owing to the complicated combinations of second order metric derivatives encoded in the Ricci scalar of the action, such a transformation yields an unwieldy expression. To `tame' the transformed action, we exploit the conformal-disformal (KG) constraint previously discovered in the study of the invariance of the massless Klein-Gordon equation under disformal transformation. The result upon its application is a surprisingly much more concise and simple action in four spacetime dimensions containing three out of four sub-Lagrangians found in the Horndeski action, and three beyond-Horndeski terms. The latter group of terms may be attributed to the kinetic dependence of the conformal and disformal factors in the Bekenstein's disformal transformation. This is consistent with a related study on the special disformal transformation of the Einstein-Hilbert action where no such beyond-Horndeski terms are found to exist. Going down to three dimensions, we find a relatively simpler resulting action but the signature of three three `extraneous' terms remains. Remarkably, we find in two dimensions the Einstein-Hilbert action to be invariant under the KG-constrained Bekenstein's disformal transformation.
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Alinea et al. (2024) studied this question.
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