MELTING of three-dimensional solids usually starts at the free surface
, which typically melts at a lower temperature than the bulk material(
1). In two dimensions the starting point of many studies is the Koster
litz-Thouless theory(2,3), in which melting is initiated through dislo
cation unbinding. Langmuir monolayers-single layers of amphiphilic mol
ecules formed at the air-water interface-should provide an ideal model
for studying melting in two dimensions. Here we show that for monolay
er crystals of fatty acids coexisting with their liquid phase, the int
erior melts before the edges. The melting of crystals under mechanical
stress is initiated along the line at which the internal stress vanis
hes. We suggest that this apparently counterintuitive result arises fr
om defect migration to the region of zero stress, where they accumulat
e and nucleate melting. These results support the idea that defects pl
ay a crucial role in melting of two-dimensional systems.