The random phase approximation (RPA) spectral function of the one-dimensional
electron band with the three-dimensional long range Coulomb interaction shows a
broad feature which is spread on the scale of the plasmon energy and vanishes
at the chemical potential. The fact that there are no quasi-particle
δ-peaks is the direct consequence of the acoustic nature of the
collective plasmon mode. This behaviour of the spectral function is in the
qualitative agreement with the angle resolved photo-emission spectra of some
Bechgaard salts. In the present work we consider the modifications in the
spectral function due to finite transverse electron dispersion. The transverse
bandwidth is responsible for the appearance of an optical gap in the long
wavelength plasmon mode. The plasmon dispersion of such kind introduces the
quasi-particle δ-peak into the spectral function at the chemical
potential. The cross-over from the Fermi liquid to the non-Fermi liquid regime
by decreasing the transverse bandwidth takes place through the decrease of the
quasi-particle weight as the optical gap in the long wavelength plasmon mode is
closing.Comment: 2 pages, 2 figures, ISCOM'0