  In this paper we introduce a simple field theoretic version of the
Carrozza-Tanasa-Klebanov-Tarnopolsky (CTKT) "uncolored" holographic tensor
model. It gives a more familiar interpretation to the previously abstract modes
of the SYK or CTKT models in terms of momenta. We choose for the tensor
propagator the usual Fermionic propagator of condensed matter, with a spherical
Fermi surface, but keep the CTKT interactions. Hence our field theory can also
be considered as an ordinary condensed matter model with a non-local and
non-rotational invariant interaction. Using a multiscale analysis we prove that
this field theory is just renormalizable to all orders of perturbation theory
in the ultraviolet regime.
