A fully dynamical and finite-lempel'dture study of the electron momenhum relaxation rate and mean free path in a coupled system of electrons and bulk LO phonons in a quantum wire structure is presented. Electmn-electron and electron-phonon interactions are eeated on an &at footing within the leading-order perturbation theoq and random-phase approximation. It is demonstrated that coupled-mode effects drastically change the tramport propties of the system at low temperatures. In panicular. the 'plasmon-like' and 'LO-phonon-like' excitations yield comparable rates which, as a consequence of the singular nahlre of the ID density of states, can be large at the threshold. This is in contrast to room temperature results where oniy the LO-phonon mode conuibutes significantly to the rate. Recent technological advances have led to the realization of electron systems confined essentially in quasi-onedimensional (QlD) structures (quantum wires). These systems, by virtue of their reduced phase space may, in principle, exhibit high carrier mobility [l] which has important implications for high-speed devices. The momentum relaxation rate W R) , r,, for an electron with axial wave vector k , is an important quantity in transport calculations