  The Schwinger-Dyson Equations (SDEs) of matrix models are known to form
(half) a Virasoro algebra and have become a standard tool to solve matrix
models. The algebra generated by SDEs in tensor models (for random tensors in a
suitable ensemble) is a specific generalization of the Virasoro algebra and it
is important to show that these new symmetries determine the physical
solutions. We prove this result for random tensors at large N. Compared to
matrix models, tensor models have more than a single invariant at each order in
the tensor entries and the SDEs make them proliferate. However, the specific
combinatorics of the dominant observables allows to restrict to linear SDEs and
we show that they determine a unique physical perturbative solution. This gives
a new proof that tensor models are Gaussian at large N, with the covariance
being the full 2-point function.
