2022
DOI: 10.1103/physrevresearch.4.033239
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Ultrafast transport and energy relaxation of hot electrons in Au/Fe/MgO(001) heterostructures analyzed by linear time-resolved photoelectron spectroscopy

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Cited by 8 publications
(12 citation statements)
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“…Our results indicate that the dynamics resulting from electron–electron interactions cannot be consistently described with an energy-independent relaxation time. Generally, we observe the decay of electronic occupation further away from the Fermi edge on similar time scales as shown in photoemission measurements. ,, However, in experiments, single collision processes cannot be isolated, and the results are naturally influenced by electron–phonon interaction and other dissipation processes as transport mechanisms. ,, …”
Section: Resultssupporting
confidence: 70%
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“…Our results indicate that the dynamics resulting from electron–electron interactions cannot be consistently described with an energy-independent relaxation time. Generally, we observe the decay of electronic occupation further away from the Fermi edge on similar time scales as shown in photoemission measurements. ,, However, in experiments, single collision processes cannot be isolated, and the results are naturally influenced by electron–phonon interaction and other dissipation processes as transport mechanisms. ,, …”
Section: Resultssupporting
confidence: 70%
“…In many cases, the temporal evolution of the density of electrons within a certain energy window is of particular interest. Experimentally, such energy-resolved electron densities are accessible with, e.g., photoemission spectroscopy. , We determine theoretically these spectral electron densities from the time- and energy-dependent distribution as n E c , normalΔ E ( t ) = E c normalΔ E / 2 E c + normalΔ E / 2 f ( E , t ) .25em D ( E ) .25em normald E yielding the density of electrons in an energy interval of width Δ E centered around a central energy E c .…”
Section: Resultsmentioning
confidence: 99%
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“…Reducing the frustration of the electron density induced by the non-thermal population, this process in turn gives rise to the slowly evolving thermal contribution (dashed lines in Figure ). The found time scale τ 2 ≈ 840 ± 55 fs agrees well with the relaxation times of the non-thermal electron population in Au reported in multiple works. ,,, The picosecond time scale is dominated by the relaxation of the electronic density to the Fermi–Dirac equilibrium albeit at an elevated temperature. It can thus be construed that the first and second terms in eq are dominated by the non-thermal ( A ) and thermal ( B ) electron-induced contributions, respectively.…”
supporting
confidence: 87%
“…The exact time scale, however, is distorted by the initial distribution of the hot-laser-excited electrons in the k-space and the exponentially decaying SPP sensitivity to the depth distribution of the perturbation. 28,37 The superdiffusive nature of the nonthermal electron transport is nonetheless strongly emphasized by the experimentally found delay t(ΔR/R| max ) value of t max ≈ 350 fs.…”
mentioning
confidence: 99%