  Group field theories are higher-rank generalizations of matrix/tensor models,
and encode the simplicial geometries of quantum gravity. In this paper, we
study the thermofield double states in group field theories. The starting point
is the equilibrium Gibbs states in group field theory recently found by Kotecha
and Oriti, based on which we construct the thermofield double state as a
"thermal" vacuum respecting the Kubo-Martin-Schwinger condition. We work with
the Weyl $C^*$-algebra of group fields, and a particular type of thermofield
double states with single type of symmetry are obtained from the squeezed
states on this Weyl algebra. The thermofield double states, when viewed as
states on the group field theory Fock vacuum, are condensate states at finite
flow parameter $\beta$. We suggest that the equilibrium flow parameters $\beta$
of this type of thermofield double states in the group field theory condensate
pictures of black hole horizon and quantum cosmology are related to the inverse
temperatures in gravitational thermodynamics.
