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Book of Abstracts Book of Abstracts - Universität Konstanz

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B - 34<br />

Relaxation Dynamics <strong>of</strong> Optically Excited States <strong>of</strong> Ag Cluster Anions<br />

74<br />

Markus Engelke, Marco Niemietz, Young Dok Kim, Gerd Ganteför<br />

Fachbereich Physik, <strong>Universität</strong> <strong>Konstanz</strong>, 78457 <strong>Konstanz</strong>, Germany<br />

http://www.clusterphysik.uni-konstanz.de/<br />

For bulk metals, optically excited electronic states can relax within few tens <strong>of</strong><br />

femtoseconds due to very fast Auger-like electron-electron scattering processes. As the size <strong>of</strong> a<br />

particle decreases, changes in relaxation dynamics <strong>of</strong> optically excited states are observed [1,2].<br />

Using Time-Resolved Two-Photon Photoemission (TR-PPE) spectroscopy, relaxation times <strong>of</strong><br />

optically excited states <strong>of</strong> Ag cluster anions consisting <strong>of</strong> less than 22 atoms (pump photon<br />

energy <strong>of</strong> 1.5 eV) were determined. For Ag18 - , Ag19 - and Ag21 - , relaxation times amount to about<br />

500 femtoseconds, which are significantly longer than those <strong>of</strong> d-metal clusters consisting <strong>of</strong><br />

less than 8 atoms [3]. The long life times <strong>of</strong> the excited states <strong>of</strong> these Ag cluster anions can be<br />

explained by lower density <strong>of</strong> states above the upper levels <strong>of</strong> the non-excited electrons within<br />

the pump photon energy in these clusters, caused by a large gap between 2s and 1f electronic<br />

shells, i.e. electronic shell configurations significantly affect the electron relaxation dynamics.<br />

-<br />

Ag18 Intensity (a.u.)<br />

References<br />

0 fs<br />

133 fs<br />

266 fs<br />

932 fs<br />

1,9 ps<br />

12,9 ps<br />

48,6 ps<br />

0 1 2<br />

Binding Energy (eV)<br />

Figure 1. TR-PPE spectra <strong>of</strong> Ag 18 - . A distinct peak can<br />

be observed at a binding energy <strong>of</strong> about 1.3 eV,<br />

accompanying broad states at higher binding energies.<br />

The state at 1.3 eV can be attributed to the excitation <strong>of</strong><br />

an electron in the HOMO to an unoccupied state. As the<br />

delay between pump and probe photons increases, the<br />

signals between 1.2eV - 2.5 eV attenuate. By assuming<br />

an exponential decay <strong>of</strong> the excited state, the lifetime is<br />

estimated to be about 420 fs.<br />

[1] J.R.R. Verlet, A.E. Bragg, A. Kammrath, O. Cheshnovsky, and D.M. Neumark,<br />

J. Chem. Phys. 121, 10015 (2004).<br />

[2] M. Niemietz, P. Gerhardt, G. Ganteför and Y. D. Kim, Chem. Phys. Lett. 380, 99 (2003).<br />

[3] N. Pontius, M. Neeb, W. Eberhardt, G. Lüttgens, P. S. Bechthold, Phys. Rev. B 67, 354251 (2003)<br />

and references therein

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