Simulating two-dimensional optical pattern formation in sodium vapor,
we show that hexagonal patterns can be unstable against their own spat
ial harmonics or subharmonics. The instability results in ultrahexagon
s or subhexagons, respectively. The formation of ultrahexagons is due
to interaction with a second solution branch with a wave number nearly
resonant to the harmonics of the primary hexagon. The mechanism of th
e instabilities is discussed on the basis of order parameter equations
obtained from symmetry considerations.