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When light hits metal nanoparticles, is it hot electrons or heat?

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Under steady illumination, almost all the light energy absorbed by a metal nanoparticle ends up heating it, and only a vanishingly small fraction creates the high-energy 'hot' electrons often credited for photocatalysis.

Source

"Hot" electrons in metallic nanostructures-non-thermal carriers or heating?

Dubi Y, Sivan Y · Light, science & applications · 2019

doi.org/10.1038/s41377-019-0199-xRead the full paper ↗81 citationscc by

Study at a glance

Design
Computational / modelling — Theory and numerics: steady-state Boltzmann equation for electrons (relaxation-time e-e collisions, Bloch-Boltzmann-Peierls e-ph collisions, photoexcitation) coupled to energy balance for electrons, phonons and environment, solved for a silver nanosphere under continuous illumination.
N
Not applicable; results are numerical solutions for model parameters of silver across a range of local field strengths.
Population
Model silver nanostructure (e.g. a small Ag sphere at its plasmon resonance) under continuous-wave illumination
Outcome
Steady-state electron distribution, its non-thermal part, electron and phonon temperatures, and the fraction of absorbed power going into non-thermal carriers

Structured fields used in claim comparison tables when every cited study has a complete layer.

What they did

The authors wrote a model for electrons in a silver nanoparticle under continuous light that includes photon absorption, electron-electron collisions and electron-lattice collisions, plus heat leaking to the surroundings. Unlike earlier work, they solved for the electron and lattice temperatures self-consistently so that energy is conserved. They then separated the electron distribution into a purely thermal part and a truly non-thermal part and tracked how the absorbed power splits between them as the light intensity changes.

What they found

The non-thermal ('hot') electrons appear as shoulders within one photon energy of the Fermi level, but at low intensity the power going into them is more than 8 orders of magnitude smaller than the power going into heating, rising only to about 10^-5 of the total at higher fields. Electron and lattice temperatures both rise linearly with intensity and stay close to each other, justifying the usual single-temperature heat model. Surprisingly, just above the Fermi energy the non-thermal part consists of holes rather than electrons, an effect of electron-phonon collisions.

The limits

What it doesn't show

It is a purely theoretical study with parameters chosen for silver at one plasmon resonance; no new experiment tests the predictions. The model neglects interband transitions, non-equilibrium phonons and field inhomogeneity inside the particle, and does not treat the high-intensity regime where the metal's permittivity would itself change. It argues that some photocatalysis results are thermal, but does not model the actual chemistry or electron transfer out of the particle.

Key terms

Hot (non-thermal) electrons
Electrons whose energies do not follow a thermal Fermi-Dirac distribution, created by absorbing photons before they share energy with other electrons.
Boltzmann equation
An equation that tracks how the distribution of particles over energies changes due to excitation and collisions.
Relaxation time approximation
A simplification in which collisions push the distribution back toward a thermal one at a set rate, which lets an electron temperature be defined unambiguously.
Two-temperature model
A description in which electrons and the lattice (phonons) each have their own temperature and exchange heat.
Fermi energy
The energy level up to which electron states are filled at zero temperature; most changes in the distribution happen near it.

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Quiz yourself

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Where does most absorbed light energy go under steady illumination, according to the model?

Common questions

If so few hot electrons are made, why do hot-electron photodetectors work?

The non-thermal population at high energies is still many orders of magnitude larger than the thermal one there, which is enough for tunnelling-based detection even though it carries a tiny share of the energy.

What does this mean for plasmonic photocatalysis claims?

The authors argue that differences in reaction rates, for example between substrates, are more likely explained by temperature rise than by hot electrons, since the hot-electron number barely depends on how well heat escapes.

Why was defining a temperature out of equilibrium a problem before?

Temperature is an equilibrium concept; using the relaxation time approximation plus energy balance lets the authors assign unique electron and phonon temperatures to the steady state.

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