Abstract. Normal incidence circularly polarized VUV radiation with energies around 23 eV creates spin polarized photoelectrons from thick layers of Rb on Pt(ll 1) and thus excites oriented 4p hole states. The preferential spin direction of the Auger electrons and its dependence upon the emission angle has been measured and is compared with the corresponding angular dependence of the primary photoelectron spin polarization also measured. Since the CVV Auger decay relates to a s a pair of valence electrons, the cross comparison of results for photoelectrons and Auger electrons studies the questions on whether photoemission and Auger decay Occur in sequence, assuming an independent two step model, and whether the valence s-electrons couple to a singlet state configuration.
PACS:79.20.Fv; 79.60.Bm a singlet state configuration or also partially to a triplet state configuration. Figure 1 shows the spin polarization of the Auger electrons averaged across the Auger peak measured [4] at rubidum thick layers on Pt(111) in normal emission versus the energy of the exciting circularly polarized VUVradiation in normal incidence, after having subtracted the unpolarized inelastic background in the spin-resolved Auger electron spectra. Figure 1 also denotes the thresholds for p_~ and pa hole creation by the photons. The p½ hole states excitect above the p± threshold decay via a Koster-Kronig transition into p] hole states [6,7]. Since 2 * • at higher photon energies phototransltlons into d states are more probable, the creation ofp~ holes with magnetic sublevels mj = +½ and ms = +~ Is preferred against creation of p~ holes with ms = -½ and rn; = -3, resultPhoton impact on solids often creates core level holes with subsequent valence electron Auger decay. In Auger spectroscopy usually the energetic position and the shape of Auger lines in spin-independent intensity spectra are studied [ 1 ]. Spin-dependent effects have been investigated experimentally in most cases with ferromagnetic material [2,3], where the electrons to be emitted are highly spin oriented in the ground state. Very recently first experimental results of spin dependent Auger emission from non-magnetic Rb-layers [4] as well as from free unoriented Ba-atoms [5] exposed to circularly polarized radiation have been reported. The spin polarized radiation creates spin polarized primary photoelectrons and thus spin oriented hole states whose decay results in spin polarized Auger electrons. It is worth noting that the Auger electrons from the CVV decay of metallic Rb-layers could not be observed for an isolated Rb atom since the alkalis only have one outermost s electron. The second s electron for the decay has to be supplied in the condensed matter by the Rb neighbours via the joint valence band. This gives rise to the question on whether they only couple to