  This paper explores the behavior of systems of cold fermions as they approach
unitarity above the critical temperature. As we move away from unitarity, by
decreasing the scattering length, the dilaton, the Goldstone boson resulting
from the spontaneous breaking of Schrodinger symmetry by the Fermi sea, becomes
gapped. At energies below this gap, the interaction between quasi-particles
will be dominated by local interactions generated by off-shell dilaton
exchange. The dilaton mass can, in turn, be related via anomaly matching, to
the scattering length and contact parameter within the confines of a systematic
expansion. We use this relation to predict the s-wave Landau parameter to be
$f=\frac{8\pi a \mu_F^2 m}{3 \hbar^4k_F^4 \tilde{C}}$ where $a$ is the
scattering length, $m$ the atomic mass and $\ \tilde {C}$ is the dimensionless
contact parameter. This prediction is valid for $\left( \frac{E_F}{E}\right)^2
\gg a k_f\gg 1$ . Given this result we predict compressibility and the
quasi-particle life-time.
