2004
DOI: 10.1063/1.1797732
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Normal Auger spectra of Br in alkali bromide molecules

Abstract: Molecular Auger electron spectra following the bromine 3d ionization in gas-phase alkali bromides and in HBr were studied both experimentally and theoretically. The AES for HBr and CsBr were measured using photoexcitation, and for LiBr, NaBr, and KBr by using electron impact. These results are compared with the theoretical spectra from nonrelativistic ab initio calculations and one-center approximation and with the spectra of Br(-), computed with the multiconfiguration Dirac-Fock method.

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Cited by 7 publications
(3 citation statements)
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References 36 publications
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“…The overall enhancement in the electron emission cross section from bromouracil compared to uracil (figures 4 and 5) may be explained by the Auger cascade effect as well as the atomic giant resonance phenomena. The vacancy created in the 3d shell of a Br atom gives rise to an Auger cascade and several electrons in the energy range between 40 and 50 eV [47] can be generated from the MNN Auger process. A part of these electrons may also be produced due to collective excitation which occurs when the 3d electrons are resonantly excited to higher excited states and finally decays by emission of several electrons.…”
Section: Ddcs Ratiosmentioning
confidence: 99%
“…The overall enhancement in the electron emission cross section from bromouracil compared to uracil (figures 4 and 5) may be explained by the Auger cascade effect as well as the atomic giant resonance phenomena. The vacancy created in the 3d shell of a Br atom gives rise to an Auger cascade and several electrons in the energy range between 40 and 50 eV [47] can be generated from the MNN Auger process. A part of these electrons may also be produced due to collective excitation which occurs when the 3d electrons are resonantly excited to higher excited states and finally decays by emission of several electrons.…”
Section: Ddcs Ratiosmentioning
confidence: 99%
“…The experiments were performed at MAX-lab (Sweden) at the I411 beamline (proposal number 20130121 [44] between 84-88 eV which have been taken into account during the fitting procedure but are not displayed explicitly. Pure monomer spectrum (not shown) was used as a reference for obtaining the Lorentzian full width at half maxima (FWHMs), the spin-orbit splitting, and the relative intensities of the monomer peaks.…”
Section: Acknowledgmentsmentioning
confidence: 99%
“…The two strongest lines at 66 eV and 13.3 eV can be assigned to the ionization of He leading to He + (1s 1 ) (IP = 24.58 eV) and ionization of the 3d shell of Br 2 (IP = 77.4 eV), respectively. The two broad lines at 45 and 30 eV are attributed to the ionization of the 3d shell of Br 2 followed by the M 4,5 N 2,3 N 2,3 and M 4,5 N 1 N 1 Auger decay [71]. Ionization to the first (He + , n = 2; IP = 65.4 eV) and second (He + , n = 3; IP = 73 eV) excited ionic shell of He leads to the two lines observed at 25.5 and 17.7 eV kinetic energy [72] whereas the strong contribution around 36 eV kinetic energy can be assigned to a sequential two-photon ionization of He due to the strong peak intensity of the FEL pulse.…”
Section: Fel-induced Coulomb Explosion Imaging Inmentioning
confidence: 96%