“…Thus, we can say that the nonlocal permittivities, proposed for metals in [56][57][58], are to some extent analogous to the permittivities of graphene, which are also spatially nonlocal but were derived on the basis of first principles of quantum electrodynamics at nonzero temperature using the formalism of polarization tensor [60,61]. It was shown that for graphene described by these permittivities there is no Casimir puzzle, i.e., the Lifshitz theory is consistent with both the experimental results [62,63] and the requirements of thermodynamics [64,65].…”