Time-resolved spectral densities of non-thermal electrons in gold
Noble-metal nanoparticles for photocatalysis have become a major research object in recent years due to their plasmon-enhanced strong light-matter interaction. The dynamics of the hot electrons in the noble metal are crucial for the efficiency of the photocatalysis and for the selective control of r...
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Main Authors | , , , , , |
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Format | Journal Article |
Language | English |
Published |
07.07.2023
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Subjects | |
Online Access | Get full text |
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Summary: | Noble-metal nanoparticles for photocatalysis have become a major research
object in recent years due to their plasmon-enhanced strong light-matter
interaction. The dynamics of the hot electrons in the noble metal are crucial
for the efficiency of the photocatalysis and for the selective control of
reactions. In this work, we present a kinetic description of the
non-equilibrium electron distribution created by photoexcitation, based on full
energy-resolved Boltzmann collision integrals for the laser excitation as well
as for the electron-electron thermalization. The laser-induced electronic
non-equilibrium and the inherently included secondary electron generation
govern the dynamics of non-thermal electrons. Applying our method to gold, we
show a significant dependence of hot electron dynamics on kinetic energy.
Specifically, the timescales of the relaxation as well as the qualitative
behavior are depending on the evaluated energy window. During the
thermalization processes there are cases of increasing electron density as well
as of decreasing electron density. Studying the influence of excitation
parameters, we find that the photon energy and the fluence of the exciting
laser can be tuned to influence not only the initial excitation but also the
subsequent characteristics of the time-resolved electronic spectral density
dynamics. The electronic thermalization including secondary electron generation
leads to time-dependent spectral densities which differ from their specific
final equilibrium values for picoseconds after irradiation ended. |
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DOI: | 10.48550/arxiv.2307.03572 |