Quasi-low-dimensional (quasi-low-D) inorganic materials are not only ideally
suited for angle resolved photoemission spectroscopy (ARPES) but also they
offer a rich ground for studying key concepts for the emerging paradigm of
non-Fermi liquid (non-FL) physics. In this article, we discuss the ARPES
technique applied to three quasi-low-D inorganic metals: a paradigm Fermi
liquid (FL) material TiTe2β, a well-known quasi-1D charge density wave
(CDW) material K0.3βMoO3β and a quasi-1D non-CDW material
Li0.9βMo6βO17β. With TiTe2β, we establish that a many body
theoretical interpretation of the ARPES line shape is possible. We also address
the fundamental question of how to accurately determine the {\bf k}Fβ value
from ARPES. Both K0.3βMoO3β and Li0.9βMo6βO17β show
quasi-1D electronic structures with non-FL line shapes. A CDW gap opening is
observed for K0.3βMoO3β, whereas no gap is observed for
Li0.9βMo6βO17β. We show, however, that the standard CDW theory,
even with strong fluctuations, is not sufficient to describe the non-FL line
shapes of K0.3βMoO3β. We argue that a Luttinger liquid (LL) model is
relevant for both bronzes, but also point out difficulties encountered in
comparing data with theory. We interpret this situation to mean that a more
complete and realistic theory is necessary to understand these data.Comment: 23 pages, including 21 figures; to appear in a special issue of J.
Elec. Spectr. Rel. Pheno