“…The combination of eqn (4b) and ( 5) implies that the relaxation rate of vorticity fluctuations is determined by the same dispersion relation that controls C > , given by eqn (8). Expanding the mode for q { l Z À1 gives a simple linear equation commonly seen in models of pattern-formation, q t ô = iO 4 (q) ô, with iO 4 (q) = À[t c À1 + k 2 q 2 + k 4 q 4 ] +O(q 6 ), (11) where k 2 = K/g + l(a + al)/(2G) and k 4 = (ÀaZl + KGl 2 À aZl 2 )/ (2G 2 ), both depend on activity. Such an equation has been used as a minimal model to study emergent structures and dynamics in active fluids, where it has been shown to support various time-independent solutions in the form of vortex lattices 34 when k 2 o 0.…”