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We show that the mimetic theory with the constraint gρσ∂ρϕ∂σϕ=1 cannot realize the black hole geometry with the horizon(s). To overcome such issue, we may change the mimetic constraint a little bit by ω(ϕ)gρσ∂ρϕ∂σϕ=−1, where ω(ϕ) is a function of the scalar field ϕ. As an example, we consider (2+1)-dimensional mimetic gravity with the mimetic potential and construct black hole (BH) solutions by using this modified constraint. We study three different classes: In the first class, we assume the Lagrange multiplier and mimetic potential are vanishing and obtain a BH solution that fully matches the BH of GR despite the non-triviality of the mimetic field which ensures the study presented in Nashed et al. (2019) 42. In the second class, we obtain a BH having constant mimetic potential and a non-trivial form of the Lagrange multiplier. In the third class, we obtain a new BH solution with non-vanishing values of the mimetic field, the Lagrange multiplier, and the mimetic potential. In any case, the solutions correspond to the space-time with only one horizon but we show that the formalism for the constraint works.
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Shin’ichi Nojiri
High Energy Accelerator Research Organization
G. G. L. Nashed
British University in Egypt
Physics Letters B
Nagoya University
British University in Egypt
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Nojiri et al. (Wed,) studied this question.
synapsesocial.com/papers/6a15644f9b87f33fc69f841c — DOI: https://doi.org/10.1016/j.physletb.2022.137140