The main purpose of this paper is to make it clear that the physical value
obtained along the trajectory generated by the new numerical scheme [J. Phy
s. Sec. Jpn. 69 (2000) 679.] satisfies the canonical distribution. On the b
asis of our proof, the scattering form factors are evaluated from the time
evolution of the spatial pattern that fluctuates around the equilibrium lam
ellar pattern. Beyond critical values of temperature, the transitions from
a lamellar pattern to hexagonal and isotropic patterns occur in the vicinit
y of the morphological transition point.