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VUV Spectroscopy of Atoms, Molecules and Surfaces

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82 Chapter 5. Femtosecond <strong>VUV</strong> core-level spectroscopy ...<br />

the technique <strong>of</strong> pico- or femtosecond X-ray diffraction, using X-rays emitted<br />

from fs laser-produced plasmas or obtained from ”sliced” or time-gated<br />

synchrotron-radiation pulses (cf. chapter 1.4). The non-thermal melting process<br />

is characterized by a disordering <strong>of</strong> the crystal lattice accomplished by<br />

the sudden excitation <strong>of</strong> a large (∼10 %) fraction <strong>of</strong> the electrons from the<br />

valence b<strong>and</strong> to the conduction b<strong>and</strong> <strong>of</strong> the semiconductor. The lattice instability<br />

occurs before a significant amount <strong>of</strong> the electronic energy has been<br />

transferred to the lattice by electron-phonon interactions <strong>and</strong> is thus purely<br />

electronic in nature. The disordering has been observed for different laser<br />

fluences encompassing the damage threshold [19, 20, 22], below which it is<br />

found to be reversible <strong>and</strong> accompanied by a b<strong>and</strong>-gap collapse for fluences<br />

near the damage threshold [23].<br />

5.2 Laser-induced desorption<br />

The field <strong>of</strong> photo-induced desorption <strong>of</strong> molecules from surfaces using pulsed<br />

laser light <strong>of</strong> nanosecond (ns) or femtosecond (fs) duration has undergone a<br />

rapid development within the last ten years as reflected by the large amount <strong>of</strong><br />

review literature available on the subject [24, 25, 26, 27, 28, 29, 30, 31, 32, 33].<br />

A chemical reaction taking place at a surface can be very different from that<br />

<strong>of</strong> the gas-phase, since the molecules are confined to aligned geometries <strong>and</strong><br />

their chemical properties are modified by the presence <strong>of</strong> the surface [29].<br />

In addition, a non-insulating surface acts as a heat-reservoir with an almost<br />

infinte number <strong>of</strong> degrees <strong>of</strong> freedom, interacting with the adsorbate <strong>and</strong><br />

representing a challenge to theorists. Since the heating- or exciting laser<br />

light penetrates several atomic layers into the substrate supporting the adsorbate<br />

layer, the desorption process is much more likely the result <strong>of</strong> an<br />

adsorbate-substrate coupling than a direct laser-adsorbate interaction. The<br />

emphasis <strong>of</strong> the present chapter is on the laser-induced desorption <strong>of</strong> diatomic<br />

molecules from metal surfaces, which are the systems that have been most<br />

intensively investigated with ns–fs laser pulses. In particular, the interest<br />

has concentrated on the catalytically- <strong>and</strong> theoretically relevant systems <strong>of</strong><br />

CO, NO or O2 molecules adsorbed on Cu, Ru, Pd or Pt surfaces. The focus<br />

<strong>of</strong> the following discussion will therefore mainly be on the information obtained<br />

from previous all-optical studies <strong>of</strong> such systems, representing a good<br />

starting point for the application <strong>of</strong> the new technique <strong>of</strong> fs <strong>VUV</strong> core-level<br />

spectroscopy. In most <strong>of</strong> the all-optical approaches the desorbed molecules<br />

have been detected in a mass spectrometer [34, 35] or by the technique <strong>of</strong><br />

Resonantly Enhanced Multi-Photon Ionization (REMPI) [36, 37, 38]. In this<br />

manner information was obtained about the translational-, vibrational- <strong>and</strong><br />

rotational distributions <strong>of</strong> the desorbed molecules <strong>and</strong> the desorption prob-

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