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Title: Adsorption of hydrogen on neutral and charged fullerene: Experiment and theory

Journal Article · · Journal of Chemical Physics
DOI:https://doi.org/10.1063/1.4790403· OSTI ID:22105385
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  1. Institut fuer Ionenphysik und Angewandte Physik, University of Innsbruck, Technikerstrasse 25, A-6020 Innsbruck (Austria)

Helium droplets are doped with fullerenes (either C{sub 60} or C{sub 70}) and hydrogen (H{sub 2} or D{sub 2}) and investigated by high-resolution mass spectrometry. In addition to pure helium and hydrogen cluster ions, hydrogen-fullerene complexes are observed upon electron ionization. The composition of the main ion series is (H{sub 2}){sub n}HC{sub m}{sup +} where m= 60 or 70. Another series of even-numbered ions, (H{sub 2}){sub n}C{sub m}{sup +}, is slightly weaker in stark contrast to pure hydrogen cluster ions for which the even-numbered series (H{sub 2}){sub n}{sup +} is barely detectable. The ion series (H{sub 2}){sub n}HC{sub m}{sup +} and (H{sub 2}){sub n}C{sub m}{sup +} exhibit abrupt drops in ion abundance at n= 32 for C{sub 60} and 37 for C{sub 70}, indicating formation of an energetically favorable commensurate phase, with each face of the fullerene ion being covered by one adsorbate molecule. However, the first solvation layer is not complete until a total of 49 H{sub 2} are adsorbed on C{sub 60}{sup +}; the corresponding value for C{sub 70}{sup +} is 51. Surprisingly, these values do not exhibit a hydrogen-deuterium isotope effect even though the isotope effect for H{sub 2}/D{sub 2} adsorbates on graphite exceeds 6%. We also observe doubly charged fullerene-deuterium clusters; they, too, exhibit abrupt drops in ion abundance at n= 32 and 37 for C{sub 60} and C{sub 70}, respectively. The findings imply that the charge is localized on the fullerene, stabilizing the system against charge separation. Density functional calculations for C{sub 60}-hydrogen complexes with up to five hydrogen atoms provide insight into the experimental findings and the structure of the ions. The binding energy of physisorbed H{sub 2} is 57 meV for H{sub 2}C{sub 60}{sup +} and (H{sub 2}){sub 2}C{sub 60}{sup +}, and slightly above 70 meV for H{sub 2}HC{sub 60}{sup +} and (H{sub 2}){sub 2}HC{sub 60}{sup +}. The lone hydrogen in the odd-numbered complexes is covalently bound atop a carbon atom but a large barrier of 1.69 eV impedes chemisorption of the H{sub 2} molecules. Calculations for neutral and doubly charged complexes are presented as well.

OSTI ID:
22105385
Journal Information:
Journal of Chemical Physics, Vol. 138, Issue 7; Other Information: (c) 2013 American Institute of Physics; Country of input: International Atomic Energy Agency (IAEA); ISSN 0021-9606
Country of Publication:
United States
Language:
English

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