A boundary condition is formulated for the interface of a quantum well embe
dded in a material of large energy barrier. Distinct differences are pointe
d out between a free-standing film and the quantum well. The boundary condi
tion for the effective-mass and envelope-function approach includes the pro
perty of the transition layer between the well and the barrier in the form
of an adjustable parameter. A full-zone k.p method is used along with the b
oundary condition to calculate the energy gap of the quantum well as a func
tion of the well thickness. The model fits well the experimental data on mu
ltiple Si/SiO2 quantum wells.