We investigate the nonequilibrium tube length fluctuations during the relax
ation of an initially stretched, entangled polymer chain. The time-dependen
t variance sigma (2) of the tube length follows in the early-time regime a
simple universal power law sigma (2) = A roott originating in the diffusive
motion of the polymer segments. The amplitude A is calculated analytically
both from standard reptation theory and from an exactly solvable lattice g
as model for reptation and its dependence on the initial and equilibrium tu
be length, respectively, is discussed. The nonuniversality suggests the mea
surement of the fluctuations (e.g., using flourescence microscopy) as a tes
t for reptation models. (C) 2001 American Institute of Physics.