We investigate the spectral properties of a non-Hermitian
quasi-one-dimensional lattice in two possible dimerization configurations.
Specifically, we focus on a non-Hermitian diamond chain that presents a
zero-energy flat band. The flat band originates from wave interference and
results in eigenstates with a finite contribution only on two sites of the unit
cell. To achieve the non-Hermitian characteristics, we introduce non-reciprocal
intrasite hopping terms in the chain. This leads to the accumulation of
eigenstates on the boundary of the system, known as the non-Hermitian skin
effect. Despite this accumulation of eigenstates, for one of the two possible
configurations, we can characterize the presence of non-trivial edge states at
zero energy by a real-space topological invariant known as the biorthogonal
polarization. We show that this invariant, evaluated using the destructive
interference method, characterizes the non-trivial phase of the non-Hermitian
diamond chain. For the other possible non-Hermitian configuration, we find that
there is a finite quantum metric associated with the flat band. Additionally,
we observe the skin effect despite having the system a purely real or imaginary
spectrum. For both configurations, we show that two non- Hermitian diamond
chains can be mapped into two models of the Su-Schrieffer-Heeger chains, either
non-Hermitian and Hermitian, in the presence of a flat band. This mapping
allows us to draw valuable insights into the behavior and properties of these
systems.Comment: 14 pages, 9 figure