We study theoretically the hexagonal phase of diblock copolymer melts
and determine the conditions under which a region of lamellar ordering
is induced near a flat surface. In the weak segregation limit we empl
oy a Landau-Ginzburg mean-field theory to describe the interfacial str
ucture of the ordered hexagonal phase. The surface field, proportional
to the differential affinity of blocks A and B to the surface, couple
s to the wave component perpendicular to the interface and increases t
he lamellar character of the ordered structure close to the surface. T
he extent of the region where this lamellar character predominates div
erges logarithmically when the hulk hexagonal-lamellar transition is a
pproached. In the strong segregation limit we find that the lamellar r
egion exists provided that the surface field is larger than some criti
cal value, readily obtainable in experiments. We find that the extent
of the region of lamellar ordering also increases logarithmically with
decreasing free energy difference between the hexagonal and lamellar
phases.