2009
DOI: 10.1088/0953-4075/42/13/134012
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EUV-photon-induced multiple ionization and fragmentation dynamics: from atoms to molecules

Abstract: Abstract:Multiple ionization (MI), induced by few VUV-photons at energies of 28.2 eV, 38 eV and 44 eV from FLASH (the free-electron laser at Hamburg), has been studied for atoms (He, Ne, Ar) and N 2 molecules utilizing our multi-hit coincident technology − the reaction microscope. At comparably low intensities of I ≅ 10 11 ∼1013 W/cm 2 we find the non-sequential (NS) MI mechanism dominating Ar 3+ and Ar 4+ production. Inspecting recoil-ion and electron momentum distributions evidence is provided (i) for pre… Show more

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Cited by 18 publications
(20 citation statements)
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“…Of course KER spectra cannot be predicted by rate equations alone, the nuclear degrees of freedom need to be considered. Experiments in the EUV on N 2 and O 2 [11][12][13] addressed the origin of different structures in the KER spectra for singly charged ions. For O 2 in [11] the number of photons absorbed was determined, and a suggestion was made for a set of electronic states involved based on the variation of the spectrum when increasing the intensity and by comparing with coincidence measurements.…”
Section: Introductionmentioning
confidence: 99%
“…Of course KER spectra cannot be predicted by rate equations alone, the nuclear degrees of freedom need to be considered. Experiments in the EUV on N 2 and O 2 [11][12][13] addressed the origin of different structures in the KER spectra for singly charged ions. For O 2 in [11] the number of photons absorbed was determined, and a suggestion was made for a set of electronic states involved based on the variation of the spectrum when increasing the intensity and by comparing with coincidence measurements.…”
Section: Introductionmentioning
confidence: 99%
“…In particular, total ionization cross sections [33,34], time-of-flight spectra [42] , as well as energy and angular distributions [44][45][46] ion yield originating from single-photon ionization, which manifests a slope of 1 in a doublelogarithmic representation (see [38,44,45]). …”
Section: Multiple Fragmentation Of N 2 Moleculementioning
confidence: 99%
“…10). The need for two photons to be absorbed is most likely due to exceedingly small cross sections close to the single-photon double ionization threshold, while sequential twophoton double ionization involving, e.g., excited states of N 2 + is expected to be relatively large [44]. Second, the asymmetric dissociative dication channel (N 2 2+ N 2+ +N) is dominated by three-photon absorption even though only two photons would be needed.…”
Section: Multiple Fragmentation Of N 2 Moleculementioning
confidence: 99%
“…For a linearly polara) Electronic mail: larsson [at] caltech.eδu; Present address: Division of Chemistry and Chemical Engineering, California Institute of Technology, Pasadena, CA 91125, USA ized field, are they accelerated to the same or to opposite directions? 2,[11][12][13][14][15][16][17][18][19][20][21] The motion into the same direction is called front-to-back or correlated motion whereas the motion into opposite directions is called back-to-back or anti-correlated motion. 2,11,13,[22][23][24] The external field couples directly only to the front-to-back motion.…”
Section: Introductionmentioning
confidence: 99%