A theory of correlated many chain motions is developed for linear chai
n polymer melts. The center of mass diffusion constant of the chains i
s shown to be inversely proportional to the number of monomers that ha
ve their motion correlated with the motion of any given monomer. This
quantity is expressed as the integral over the normalized correlation
function for the displacements of different monomers in the melt. Two
limiting cases are considered for this correlation function in monodis
perse melts. The loss of correlation in the motion of monomers occurs
because of the relative motion of the chains. The first limiting case
assumes that the relative chain motions are correlated over the entire
range of the correlated many chain motion. This case leads to the lar
gest single contribution to the diffusion constant in the long chain l
imit. The second limiting case employs the shortest possible correlati
on length for the relative displacements of the chains. Since this cas
e allows for the greatest randomness in the motion of the chains, it i
s expected that the contribution from this type of correlated motion s
hould dominate the chain diffusion constant. The diffusion constant ba
sed on the correlated motions in the melt is consistent with the exper
imentally observed chain length scaling of both the terminal time and
the chain diffusion constant. The case of the diffusion of a single pr
obe chain in a melt of host chains of different length is also discuss
ed. (C) 1995 American Institute of Physics.