We calculate the lamellar period L and interphase thickness a of an in
compressible melt of symmetric diblock copolymers from the onset of ph
ase segregation (weak segregation limit) to the limit where segregatio
n is almost complete (strong segregation limit) by numerically solving
a mean field lattice model, where the lattice spacing is taken small
enough to approximate a continuum. Our results for L and a agree with
previously derived theoretical formulas in both limits. Based on the f
irst few terms of a Fourier series expansion of the density profile, w
e show analytically that L = 0.844R(chi(N))0.571 at the weak segregati
on limit, where R is the unperturbed molecular radius of gyration, chi
the Flory interaction parameter, and N the number of statistical segm
ents per molecule; the compressibility of the melt-even in the incompr
essible limit-must be taken into consideration to get the correct depe
ndence of L on chi(N), and the Fourier series approximation turns out
to be accurate over a very small range of chi(N).