2020
DOI: 10.3390/atoms8030045
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Photoionization of Astrophysically Relevant Atomic Ions at PIPE

Abstract: We review recent work on the photoionization of atomic ions of astrophysical interest that has been carried out at the photon-ion merged-beams setup PIPE, a permanently installed end station at the XUV beamline P04 of the PETRA III synchrotron radiation source operated by DESY in Hamburg, Germany. Our results on single and multiple L-shell photoionization of Fe+, Fe2+, and Fe3+ ions, and on single and multiple K-shell photoionization of C−, C+, C4+, Ne+, and Si2+ ions are discussed in astrophysical contexts. M… Show more

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Cited by 12 publications
(9 citation statements)
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References 109 publications
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“…The experiment was performed at the end station PIPE (Schippers et al 2014;Müller et al 2017; of the photon beamline P04 (Viefhaus et al 2013) at the synchrotron light source PETRA III, which is operated by DESY in Hamburg, Germany. As for our previous work on L-shell photoionization of Fe + and Fe 3+ (Schippers et al 2017;Beerwerth et al 2019), we have employed the photon-ion merged-beams technique (for recent overviews, see Schippers et al 2016b;Schippers & Müller 2020) to measure cross sections for single and multiple photoionization of Fe 2+ ions. The experimental photon-energy range was 690-920eV.…”
Section: Methodsmentioning
confidence: 99%
“…The experiment was performed at the end station PIPE (Schippers et al 2014;Müller et al 2017; of the photon beamline P04 (Viefhaus et al 2013) at the synchrotron light source PETRA III, which is operated by DESY in Hamburg, Germany. As for our previous work on L-shell photoionization of Fe + and Fe 3+ (Schippers et al 2017;Beerwerth et al 2019), we have employed the photon-ion merged-beams technique (for recent overviews, see Schippers et al 2016b;Schippers & Müller 2020) to measure cross sections for single and multiple photoionization of Fe 2+ ions. The experimental photon-energy range was 690-920eV.…”
Section: Methodsmentioning
confidence: 99%
“…Because of the many-body nature of the theoretical problem, the theoretical calculations have to resort to approximations yielding results that bear (usually unknown) uncertainties. In this situation, benchmarking by laboratory experiments (Schippers & Müller 2020) is vital for arriving at sufficiently accurate results that allow one, in the present context, to reliably discriminate between the gaseous and solid components of the ISM.…”
Section: Introductionmentioning
confidence: 99%
“…Because of the many-body nature of the theoretical problem the theoretical calculations have to resort to approximations yielding results that bear (usually unknown) uncertainties. In this situation, benchmarking by laboratory experiments (Schippers & Müller 2020) is vital for arriving at suffi-ciently accurate results that allow one, in the present context, to reliably discriminate between the gaseous and solid components of the ISM.…”
Section: Introductionmentioning
confidence: 99%