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Diploma - Max Planck Institute for Solid State Research

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17<br />

3 Experimental foundations<br />

3.1 Photoemission<br />

Having already regarded the principles of photoemission (see ch. 2.2) this paragraph<br />

concentrates on experimental issues. At least, one has to note the following effects and<br />

differences:<br />

• To obtain angle-resolved spectra high-quality monocrystalline samples are needed<br />

because the translational invariance is a requirement <strong>for</strong> momentum conservation<br />

in photoemission.<br />

• Since the incident photon beam has a finite spot size, we have spatial as well<br />

as temporal integration <strong>for</strong> the outgoing particle wave functions in addition to<br />

the intrinsic interference contribution of different PE channels. Furthermore, the<br />

sample’s surface is not homogeneous (breaking exactly at one well defined layer)<br />

and exhibits terraces and single atoms adsorbed at the surface. Additionally, the<br />

sample can have different oriented domains and there<strong>for</strong>e one usually integrates<br />

(spatially) over a non-homogeneous surface region (we selected samples whith<br />

large single-domain regions <strong>for</strong> PE).<br />

• Having a semi-infinite solid, we face in principle three different states (cf. fig. 2.6)<br />

which are crucial <strong>for</strong> photoemission: bulk states, surface resonances and surfaces<br />

states (the last two will be subsumed as surface states). Given that the<br />

Figure 3.1: manipulator including sample holder inside the preparation chamber: left: raw<br />

sample with lever stick; right: cleaved sample

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