Extensive molecular dynamics simulations are carried out to study static an
d dynamic properties of symmetric diblock copolymer melts, both in the diso
rdered and in the lamellar phases. The lamellar phase is constructed using
the natural lamellar spacing, determined from constant pressure simulations
. The non-Gaussian character of the chains in the disordered phase is demon
strated and quantified. In the lamellar phase, the density profile of the s
eparate blocks, as well as the interface thickness are determined as a func
tion of chain length N and AB interaction parameter <(epsilon)over tilde>,
and compared with experiments and other theoretical results. Single chain a
nd single block form factors indicate that the chains in the lamellar phase
are distorted into stick-like objects. Our results in the disordered phase
show a stronger dependence of the diffusion constant on the chain length t
han observed in previous simulations. Diffusion within the lamellar plane f
or systems with chains of length N less than or equal to 100 monomers is fo
und to be almost independent of <(epsilon)over tilde>, in agreement with th
e predictions by Barrat and Fredrickson for Rouse chains. Diffusion perpend
icular to the lamellae is exponentially suppressed with increasing <(epsilo
n)over tilde>. Simulations with even longer chains (up to N = 400 monomers)
indicate that, in the strong segregation regime, chain stretching lowers t
he entanglement density and shifts the tube motion characteristic of the ch
ain dynamics in homogeneous melts of long chains toward much longer chains.