Structural transformations on elemental semiconductor surfaces typical
ly occur above several hundred degrees Celsius, and the atomic motions
involved are extremely rapid and difficult to observe. However, on th
e (111) surface of germanium, a few lead atoms catalyze atomic motions
so that they can be observed with a tunneling microscope at temperatu
res below 80 degrees C. Mass transport and structural changes are caus
ed by the creation and propagation of both vacancy-like and interstiti
al-like point defects within the crystal surface. The availability of
dangling bonds on the surface is critical. A detailed atomic model for
the observed motions has been developed and is used to explain the st
ructural phase transition Ge(111)-c(2x8) <----> 1 x 1, which occurs ne
ar 300 degrees C.