The intense fields in laser pulses produce a wide variety of nonpertur
bative and nonlinear effects within individual atoms or molecules (e.g
., harmonic generation, multiphoton ionization, etc.). Aggregates of a
toms (e.g., vapors, clusters, metals, glass, etc.) subject to intense
pulses exhibit a variety of breakdown (or damage) phenomena that deriv
e from the strong-field effects in individual atoms and the collective
effect of bulk matter. We review some of these connections, with part
icular emphasis on recent investigations in our laboratory of short-pu
lse laser-induced changes to transparent dielectric solids. Although t
he phenomena of laser-induced breakdown and damage have great complexi
ty in general and requires elaborate details ranging from electron col
lision physics to strength of materials and fracture, simplifications
become possible for short pulses. In particular, the brevity of the la
ser pulse implies that the threshold for material damage is primarily
determined by conduction electrons. We comment on the implications of
the simplifying physics that becomes applicable for short pulses, and
the consequences of this simplification both for theoretical modeling
and for useful applications.