Absorption spectra at the iodine 3d ionisation threshold following the CH x I + ( x = 0–3) cation sequence

Yields of atomic iodine I q+ ( q ≥ 2) fragments resulting from photoexcitation and photoionisation of the target cations CH x I + ( x = 0–3) have been measured in the photon-energy range 610 eV to 670 eV, which comprises the threshold for iodine 3d ionisation. The measured ion-yield spectra show two...

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Veröffentlicht in:Physical chemistry chemical physics : PCCP 2019-11, Vol.21 (45), p.25415-25424
Hauptverfasser: Schubert, Kaja, Guda, Alexander A., Mertens, Karolin, Schunck, Jan O., Schippers, Stefan, Müller, Alfred, Bari, Sadia, Klumpp, Stephan, Martins, Michael
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container_end_page 25424
container_issue 45
container_start_page 25415
container_title Physical chemistry chemical physics : PCCP
container_volume 21
creator Schubert, Kaja
Guda, Alexander A.
Mertens, Karolin
Schunck, Jan O.
Schippers, Stefan
Müller, Alfred
Bari, Sadia
Klumpp, Stephan
Martins, Michael
description Yields of atomic iodine I q+ ( q ≥ 2) fragments resulting from photoexcitation and photoionisation of the target cations CH x I + ( x = 0–3) have been measured in the photon-energy range 610 eV to 670 eV, which comprises the threshold for iodine 3d ionisation. The measured ion-yield spectra show two strong and broad resonance features due to the excitation of the 3d 3/2,5/2 electrons into ε f states similar to atomic iodine. In the 3d pre-edge range, electrons are excited into molecular orbitals consisting of iodine, carbon, and hydrogen atomic orbitals. These transitions have been identified by comparison with literature data and by simulations using time-dependent density functional theory (TDDFT) with the KMLYP functional. The ion-yield spectrum for CH 3 I + resembles the spectrum of IH + [Klumpp et al. , Phys. Rev. A , 2018, 97 , 033401] because the highest occupied molecular orbitals (HOMO) of the H and CH 3 fragments both contain a single vacancy, only. For the molecular cations with higher number of vacancies in the valence molecular orbitals CH x I + ( x = 0–2), a stronger hybridisation of the molecular orbitals occurs between the organic fragment and the iodine resulting in a change of bonding from a single σ bond in CH 3 I + to a triple bond including two π orbitals in CI + . This is reflected in the resonance energies of the observed absorption lines below the iodine 3d excitation threshold.
doi_str_mv 10.1039/C9CP04640B
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The measured ion-yield spectra show two strong and broad resonance features due to the excitation of the 3d 3/2,5/2 electrons into ε f states similar to atomic iodine. In the 3d pre-edge range, electrons are excited into molecular orbitals consisting of iodine, carbon, and hydrogen atomic orbitals. These transitions have been identified by comparison with literature data and by simulations using time-dependent density functional theory (TDDFT) with the KMLYP functional. The ion-yield spectrum for CH 3 I + resembles the spectrum of IH + [Klumpp et al. , Phys. Rev. A , 2018, 97 , 033401] because the highest occupied molecular orbitals (HOMO) of the H and CH 3 fragments both contain a single vacancy, only. For the molecular cations with higher number of vacancies in the valence molecular orbitals CH x I + ( x = 0–2), a stronger hybridisation of the molecular orbitals occurs between the organic fragment and the iodine resulting in a change of bonding from a single σ bond in CH 3 I + to a triple bond including two π orbitals in CI + . 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The measured ion-yield spectra show two strong and broad resonance features due to the excitation of the 3d 3/2,5/2 electrons into ε f states similar to atomic iodine. In the 3d pre-edge range, electrons are excited into molecular orbitals consisting of iodine, carbon, and hydrogen atomic orbitals. These transitions have been identified by comparison with literature data and by simulations using time-dependent density functional theory (TDDFT) with the KMLYP functional. The ion-yield spectrum for CH 3 I + resembles the spectrum of IH + [Klumpp et al. , Phys. Rev. A , 2018, 97 , 033401] because the highest occupied molecular orbitals (HOMO) of the H and CH 3 fragments both contain a single vacancy, only. 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The measured ion-yield spectra show two strong and broad resonance features due to the excitation of the 3d 3/2,5/2 electrons into ε f states similar to atomic iodine. In the 3d pre-edge range, electrons are excited into molecular orbitals consisting of iodine, carbon, and hydrogen atomic orbitals. These transitions have been identified by comparison with literature data and by simulations using time-dependent density functional theory (TDDFT) with the KMLYP functional. The ion-yield spectrum for CH 3 I + resembles the spectrum of IH + [Klumpp et al. , Phys. Rev. A , 2018, 97 , 033401] because the highest occupied molecular orbitals (HOMO) of the H and CH 3 fragments both contain a single vacancy, only. 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title Absorption spectra at the iodine 3d ionisation threshold following the CH x I + ( x = 0–3) cation sequence
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