
Plasmon Losses in XPS #
When an X-ray photon ejects a core-level electron from a solid, the outgoing photoelectron can interact with the material’s electron cloud.
This interaction can excite plasmons—quantized oscillations of the conduction electrons (often called Langmuir waves).
As a result, some photoelectrons lose additional energy equal to one or more plasmon quanta before escaping the material.
These energy losses appear as satellite peaks (plasmon loss peaks) at fixed energy intervals (the plasmon energy) on the higher binding energy (lower kinetic energy) side of the main photoelectron peak.

Mg metal by XPS with plasmon peaks labelled
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Intrinsic Plasmon Peaks:
Arise when the photoelectron excites a plasmon at the point of photoemission (inside the atom or molecule). -
Extrinsic Plasmon Peaks:
Occur when the photoelectron excites a plasmon as it travels through the solid towards the surface. -
Bulk Plasmon Peaks:
Collective oscillations of the free electron gas inside the bulk of a material. -
Surface Plasmon Peaks:
Collective oscillations of electrons localized at the surface of a material, particularly at the interface between a conductor (often a metal) and a dielectric (such as air or vacuum).
Plasmon peaks in XPS serve as powerful tools for material characterization, as their presence, position, and intensity can be used to identify specific materials, assess their purity, and probe key electronic properties such as electron density and conductivity. The energy and shape of these peaks are characteristic of the material’s electronic structure, allowing researchers to distinguish between different compounds or detect impurities that alter the plasmon response. Beyond basic identification, the detailed analysis of plasmon peaks provides valuable insights into surface and nanostructure features. For instance, variations in the intensity or broadening of plasmon peaks can indicate changes in surface roughness, the formation of nanostructures, or the existence of thin films and nanoparticles, since these factors influence how collective electron oscillations are excited and dissipated. Furthermore, careful recognition and interpretation of plasmon loss features are essential for accurate spectral analysis in XPS. Plasmon peaks often appear close to or overlapping with core-level photoelectron peaks, and if not properly accounted for, they can distort quantitative measurements or lead to misassignment of chemical states. Thus, understanding plasmon-related features is critical not only for extracting meaningful electronic and structural information but also for ensuring the reliability of XPS data interpretation.