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Diploma - Max Planck Institute for Solid State Research

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57<br />

5 Summary<br />

In this diploma thesis angle-resolved photoemission spectroscopy and density functional<br />

theory based calculations have been used to study the ternary rare-earth compound<br />

EuRh 2 Si 2 . Thereby the emphasis was laid on many-body interactions exploring the<br />

interplay of two opposing limits <strong>for</strong> the description of electrons: itinerant character vs.<br />

localization. Symmetry dependencies of photoemission as depicted in fig. 5.1 have been<br />

neglected.<br />

The crystal cleaves solely along the Eu–Si planes which has been demonstrated theoretically<br />

by <strong>for</strong>ce-minimization. The amount of europium atoms at the surface of the<br />

sample is not controllable, there<strong>for</strong>e one has to search <strong>for</strong> regions at the surface which<br />

are predominantly terminated by Si or Eu atoms. The kind of termination may be<br />

identified by the surface component of the Eu 4f emission which is shifted by approximately<br />

1 eV to higher binding energies whereat it is missing <strong>for</strong> Si termination. On<br />

the other hand, a star-like surface state centered around the M-point of the quadratic<br />

surface BZ located in a gap of the projected Fermi surface manifests Si termination in<br />

agreement with results of slab calculations. For the first time, a linear dispersive Diraclike<br />

state around the Γ-point has been observed <strong>for</strong> a rare earth compound. It seems<br />

to be of surface origin and has its nodal point close above (below) the Fermi energy at<br />

Si (Eu) terminated surfaces. This observation is in accordance with the surface calculations<br />

(4f treated as core orbitals) indicating that the pertubation of the eigenvalues due<br />

Figure 5.1: PE spectra<br />

of EuRh 2 Si 2 with<br />

Si termination <strong>for</strong> different<br />

polarisations<br />

at hν = 100 eV and<br />

T ≈ 2 K, aligned roughly<br />

in X − Γ − X direction<br />

(1 3 ARPES (BESSYII))<br />

(a) has been measured<br />

with horizontal polarisation<br />

and (b) with linear<br />

vertical polarisation. In<br />

comparison to SLS-SIS<br />

the polarization effect<br />

seems to be swapped<br />

(cf. fig. 4.8a)

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