Abstract
In the framework of metric-affine gravity, we consider the role of the boundary term in Symmetric Teleparallel Gravity assuming f(Q, B) models where f is a smooth function of the non-metricity scalar Q and the related boundary term B. Starting from a variational approach, we derive the field equations and compare them with respect to those of f(Q) gravity in the limit of Brightarrow 0. It is possible to show that f(Q,B)=f(Q-B) models are dynamically equivalent to f(R) gravity as in the case of teleparallel f(tilde{B}-T) gravity (where Bne tilde{B}). Furthermore, conservation laws are derived. In this perspective, considering boundary terms in f(Q) gravity represents the last ingredient towards the Extended Geometric Trinity of Gravity, where f(R), f(T,tilde{B}), and f(Q, B) can be dealt under the same standard. In this perspective, we discuss also the Gibbons–Hawking–York boundary term of General Relativity comparing it with B in f(Q, B) gravity.
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