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VUV Spectroscopy of Atoms, Molecules and Surfaces

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3.1 Introduction 45<br />

Cross section (arb. units)<br />

200<br />

150<br />

100<br />

50<br />

0<br />

10.92 10.94 10.96 10.98 11.00<br />

600<br />

400<br />

200<br />

0<br />

10.927 10.928<br />

60<br />

(b) (c)<br />

40<br />

20<br />

0<br />

Photon energy (eV)<br />

(a)<br />

10.9550 10.9555<br />

Figure 3.1: (a) Relative photodetachment cross section <strong>of</strong> D− in the vicinity <strong>of</strong> the<br />

D(n=2) threshold measured by Andersen et al. [13] <strong>and</strong> normalized to the theoretical<br />

results <strong>of</strong> Lindroth [13]. The scanned energy range includes the 2 {0} −<br />

3 <strong>and</strong> 2 {0}− 4 Feshbach<br />

resonances <strong>and</strong> the 2 {0} +<br />

2 shape resonace. (b) The 2 {0}− 3 resonance shown on an<br />

enlarged scale, fitted to a Fano pr<strong>of</strong>ile convolved with a Gaussian function representing the<br />

experimental resolution. (c) The 2 {0} −<br />

4 resonance shown on an enlarged scale, fitted to a<br />

Gaussian function.<br />

<strong>of</strong> the 2 {0} + 2 shape resonance, which appears non-smooth due to variations in<br />

the laser- <strong>and</strong> ion-beam overlap. This is a consequence <strong>of</strong> the large scaling in<br />

ion-beam energy required to scan the relatively broad photon-energy range<br />

covered by this structure. The measured cross section is relative, <strong>and</strong> each<br />

<strong>of</strong> the three segments has been normalized to the cross section calculated by<br />

Lindroth <strong>and</strong> convolved with the experimental resolution (solid curve). The<br />

2 {0}−3 <strong>and</strong> 2 {0}−4 resonances are shown on an enlarged scale in figures 3.1

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