The determination of optical constants
of noble metals that govern
the characteristics of the system has been found to be extremely important
to retrospect the observed optical properties from theoretical perspectives
to excavate the light–matter interaction at the bottom. Numerous
experimental and theoretical approaches, often, followed by fitting
through a specified model have been adopted in the literature to evaluate
the optical constants either at the bulk, thin film, or nanoscale
dimensions. Bulk optical constants have, often, been used for simulation
of the optical extinction of noble metal clusters of arbitrary sizes.
In 1900, Paul Drude proposed his model of free-electron conduction
in a metal that allows expressing the plasmonic characteristics as
a function of the common observables. Noble metals, like copper, silver,
and gold, at the nanoscale dimension exhibit a characteristic strong
absorption band in the UV–vis–NIR spectral region that
can be ascribed to the localized surface plasmon resonance (LSPR)
that is specific to nanostructures because of geometrical confinement
effects of the free electrons. The spectral position and magnitude
of the LSPR are, explicitly, governed by the density of conduction
electrons, the effective electron mass, and the shape and the size
of the charge distribution that can, solely, be attributed to the
dielectric properties of both the materials and the surrounding medium.
Prudent advances in the synthetic strategies have opened up avenues
to achieve desired nanostructures with similar morphologies and stabilizing
ligand shells dispersed under analogous conditions. The exquisite
sensitivity of the plasmonic response under varieties of microenvironmental
conditions could be employed to determine the optical constants of
the corresponding metallic nanostructures. A comparative account of
the plasmonic sensitivity of materials that requires the determination
of the dielectric constant at the nanoscale dimension has been elucidated.