Secondary instabilities of Faraday waves show three regimes: 1) As see
n previously, low-viscosity (v) fluids destabilize first into squares.
At higher driving accelerations a, squares show low-frequency modulat
ions corresponding to the motion of phase defects, while theory predic
ts a stationary transverse amplitude modulation (TAM). 2) High-v fluid
s destabilize first to stripes. Stripes then show an oscillatory TAM w
hose frequency is incommensurate with the driving frequency. At higher
a, the TAM undergoes a phase instability. At still higher a, edge dis
locations form and fluid droplets are ejected. 3) Intermediate-v fluid
s show a complex coexistence of squares and stripes, as well as statio
nary and oscillatory TAM instabilities of the stripes.