A novel undulator-based PGM beamline for circularly polarised synchrotron radiation at BESSY II

Sawhney, Kawal; Senf, F.; Scheer, M.; Schäfers, F.; Bahrdt, J.; Gaupp, A.; Gudat, W.

doi:10.1016/s0168-9002(97)00402-6

Cited by 117 publications

(68 citation statements)

References 26 publications

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“…The experiments were performed at beamline U49/2 PGM 2 [11] at the BESSY-II storage ring, Germany, using essentially the same setup as has previously been described (see, e.g., Ref. [12] and references therein).…”

Section: Methodsmentioning

confidence: 99%

Multielectron coincidence study of the double Auger decay of3d-ionized krypton

et al. 2010

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This is the published version of a paper published in Physical Review A. Atomic, Molecular, and Optical Physics. Citation for the original published paper (version of record):Andersson, E., Fritzsche, S., Linusson, P., Hedin, L., Eland, J H. et al. (2010) Multielectron coincidence study of the double Auger decay of 3d-ionized krypton.Physical Review A. Atomic, Molecular, and Optical Physics, 82(4) Multielectron coincidence data for triple ionization of krypton have been recorded above the 3d ionization threshold at two photon energies (140 and 150 eV). Three principal transition pathways have been observed, two involving double Auger transitions from Kr + , and one involving single Auger transitions from Kr 2+ created by direct single-photon double ionization. The decay of the 3d 9 2 D 5/2,3/2 states in Kr + has been analyzed in some detail and is found to be strongly dominated by cascade processes where two electrons with well-defined energies are emitted. The decay paths leading to the 4s 2 4p 3 4 S, 2 D, and 2 P states of Kr 3+ are analyzed and energies of seven intermediate states in Kr 2+ are given. A preliminary investigation of the decay paths from Kr + 3d 9 4p 5 nl shake-up states has also been carried out.

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Section: Methodsmentioning

confidence: 99%

Multielectron coincidence study of the double Auger decay of3d-ionized krypton

et al. 2010

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“…This instrument was installed on the UE56/2-PGM-2 beamline of BESSY II which comprises a 56 mm period undulator followed by a plane grating monochromator [29]. Different electron emission directions can be detected by rotating the sample about its surface normal (to change the azimuthal angle) and about a vertical axis (to change the polar angle).…”

Section: Methodsmentioning

confidence: 99%

Adsorption structure of glycine on TiO2(1 1 0): A photoelectron diffraction determination

et al. 2009

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“…This instrument was installed on the UE56/2-PGM-2 beamline of BESSY II which comprises a 56 mm period undulator followed by a plane grating monochromator [15]. Different electron emission directions can be detected by rotating the sample about its surface normal (to change the azimuthal angle) and about a vertical axis (to change the polar angle).…”

Section: Methodsmentioning

confidence: 99%