  We analyze dynamics of chiral gauge theories based on the $SU(N)$ gauge group
with one anti-symmetric tensor $A$ and $(N-4)$ anti-fundamentals $F_{i}$ when
$N$ is odd. Based on the continuity to the supersymmetric gauge theories with
anomaly-mediated supersymmetry breaking, we claim that the global $SU(N-4)$
symmetry is spontaneously broken to $Sp(N-5)$. There are $N-5$ massless
fermions as a fundamental representation of $Sp(N-5)$, and another massless
fermion, together saturating the anomaly matching conditions. When $N$ is even,
the unbroken flavor symmetry is $Sp(N-4)$ while there are no massless fermions.
Our result is different from the dynamics suggested by tumbling where the full
$SU(N-4)$ symmetry is unbroken, but the tumbling picture can be modified via
the addition of a second condensate to produce the symmetry breaking pattern
predicted from our method.
