2020
DOI: 10.1038/s42005-020-00442-x
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Parametric dependence of hot electron relaxation timescales on electron-electron and electron-phonon interaction strengths

Abstract: Understanding how photoexcited electron dynamics depend on electron-electron (e-e) and electron-phonon (e-p) interaction strengths is important for many fields, e.g. ultrafast magnetism, photocatalysis, plasmonics, and others. Here, we report simple expressions that capture the interplay of e-e and e-p interactions on electron distribution relaxation times. We observe a dependence of the dynamics on e-e and e-p interaction strengths that is universal to most metals and is also counterintuitive. While only e-p … Show more

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Cited by 31 publications
(43 citation statements)
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References 62 publications
(165 reference statements)
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“…This value is roughly 10 times lower than the energy transfer coefficient between Au electrons and Au phonons. The electron-phonon energy transfer coefficient in Au is proportional to the rate of spontaneous phonon emission by a hot electron [45]. Therefore, we estimate the rate of REIG magnon emission by hot electrons in proximity to the interface is roughly one order of magnitude lower than the rate of Au phonon emission.…”
Section: Discussionmentioning
confidence: 82%
“…This value is roughly 10 times lower than the energy transfer coefficient between Au electrons and Au phonons. The electron-phonon energy transfer coefficient in Au is proportional to the rate of spontaneous phonon emission by a hot electron [45]. Therefore, we estimate the rate of REIG magnon emission by hot electrons in proximity to the interface is roughly one order of magnitude lower than the rate of Au phonon emission.…”
Section: Discussionmentioning
confidence: 82%
“…Here, we focus on momentum changes and the net effect of the scattering between electrons and nuclei by assuming a constant characteristic time τ el . We will analyse the dynamics for two values: τ el = 25 fs taken from [29], which was used to study spin transport and spin dynamics in [9,30], and τ el = 12 fs from [31,32]. We will not take into account the loss of energy due to recoil for this simulation but focus solely on the change of the direction of flight.…”
Section: Elastic Scattering: Electron-nucleus Interactionmentioning
confidence: 99%
“…[29] and τ el = 12 fs from Ref. [30]. We will not take into account the loss of energy due to recoil for this simulation.…”
Section: Elastic Scattering: Electron -Nucleus Interactionmentioning
confidence: 99%