We analytically establish the role of a spectrum of Lyapunov exponents in the
evolution of phase-space distributions ρ(p,q). Of particular interest is
λ2, an exponent which quantifies the rate at which chaotically
evolving distributions acquire structure at increasingly smaller scales and
which is generally larger than the maximal Lyapunov exponent λ for
trajectories. The approach is trajectory-independent and is therefore
applicable to both classical and quantum mechanics. In the latter case we show
that the ℏ→0 limit yields the classical, fully chaotic, result for the
quantum cat map.Comment: 5 RevTeX pages + 2 ps figs. Phys. Rev. E (to appear,'97