Related Experiment Video
Updated: Oct 19, 2026

Experimental Methods for Spin- and Angle-Resolved Photoemission Spectroscopy Combined with Polarization-Variable Laser
Published on: June 28, 2018
Experimental and Computational Investigations of Surface Polaritons at Metal-Oxide-Semiconductor Interfaces
Humaira Zafar1, Qiang Zhang2, Rainer Straubinger2
1Department of Physics Khalifa University Abu Dhabi UAE.
Abstract:
Planar surface plasmon polaritons (SPPs) at metal-oxide-semiconductor (MOS) interfaces are central to plasmon-assisted optoelectronic and tunneling devices, where ultrathin dielectrics govern field confinement and energy transfer. However, a direct link between electron energy-loss spectroscopy (EELS) measurements and electromagnetic power dissipation at buried interfaces remains unclear. Here, we combine STEM-EELS with full-wave electromagnetic simulations to investigate SPP excitation in planar and stacks with 10 nm dielectric spacers. Using a finite-difference time-domain approach, the fast electron is modeled as a broadband electromagnetic source, enabling decomposition of extinction into absorbed and scattered power and direct comparison with EEL spectra. We show that extinction is dominated by non-radiative absorption, confirming that the observed resonances originate from SPPs confined to the buried Au-oxide interface. Increasing dielectric permittivity induces a redshift and modifies modal confinement, while losses remain Au-dominated. Kramers-Kronig analysis and simulations further confirm dielectric dispersion effects and exponential evanescent decay across the oxide layer.
Related Concept Videos
Metal-Semiconductor Junctions
Schottky Barriers
Schottky barriers arise when a metal with a work function (Φm) contacts a semiconductor with a different work function (Φs). Initially, electrons transfer until the Fermi levels of the metal and semiconductor align at equilibrium. For instance, if Φm > Φs, the semiconductor Fermi level is higher than the metal's before contact. The semiconductor's...
Potential Due to a Polarized Object
The Electrical Double Layer

