Fig. 6 | Nature Communications

Fig. 6

From: Determination of hot carrier energy distributions from inversion of ultrafast pump-probe reflectivity measurements

Fig. 6

Changes in carrier population for the Kretschmann configuration. a Spectrum cuts of Δf(E), inferred from the second integral Eq. (4), at t = 136, 163, 400 fs. The relatively broad initial electron energy distribution change at the earlier time (136 fs) evolves to a narrower and larger magnitude Fermi–Dirac distribution at later time (400 fs). b Same as a but with multiplication factors in order to better compare the various time functional forms

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