Issue |
J. Phys. IV France
Volume 114, April 2004
|
|
---|---|---|
Page(s) | 95 - 97 | |
DOI | https://doi.org/10.1051/jp4:2004114018 |
J. Phys. IV France 114 (2004) 95
DOI: 10.1051/jp4:2004114018
Effects of transverse electron dispersion on photo-emission spectra of quasi-one-dimensional systems
Z. Agic1, P. Zupanovic1 and A. Bjelis21 Faculty of Natural Sciences, Mathematics and Education, University of Split, N. Tesle 12, 21000 Split, Croatia
e-mail: agicz@pmfst.hr; pasko@pmfst.hr
2 Faculty of Science, University of Zagreb, Bijenicka 32, 10000 Zagreb, Croatia
e-mail: bjelis@phy.hr
Abstract
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
-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
-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.
Key words. plasmon - spectral function - transverse bandwidth.
© EDP Sciences 2004