A new technique is described, where picosecond laser pulses generate a
nd probe 4.2 GPa nanoshocks in polymeric and polycrystalline solids at
a high repetition rate of similar to 100/s. The term nanoshock refers
to the short duration (a few ns) of the shock pulse and the very smal
l shocked volume (a few ng). The nanoshock wave form is characterized
by the shock front risetime, shock falltime, peak pressure, and veloci
ty. Coherent Raman spectroscopy during nanoshock propagation in a 700-
nm-thick layer of polycrystalline anthracene, called an optical nanoga
uge, is used to determine these quantities. A powerful method of analy
sis, singular value decomposition (SVD), is applied to Raman spectrosc
opy of shock waves for the first time. Using SVD analysis, the risetim
e of the nanoshock pulses is found to be less than 25 ps, and the velo
city of the shook front in the nanogauge is monitored in real time. So
me possible applications of nanoshock technology in the areas of shock
-induced material transformation and shock-induced mechanical deformat
ion processes, are discussed briefly. (C) 1997 American Institute of P
hysics.