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Volumn 130, Issue 16, 2009, Pages

Non-IPR C60 solids

Author keywords

[No Author keywords available]

Indexed keywords

BAND GAPS; ELECTRON IMPACTS; ELECTRONIC MODIFICATIONS; FULLERENE CAGES; INCIDENT IONS; INTER-MOLECULAR BONDINGS; ISOMER MIXTURES; LOW-ENERGY ION BEAMS; MASS CHANNELS; MASS SPECTROMETRIC DETECTIONS; PHOTOELECTRON SPECTRUM; THERMAL STABILITIES; TRIPLET FEATURES; ULTRAVIOLET PHOTOELECTRON SPECTRUM; VAN DER WAALS;

EID: 65149098455     PISSN: 00219606     EISSN: None     Source Type: Journal    
DOI: 10.1063/1.3120287     Document Type: Article
Times cited : (17)

References (41)
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    • DFT calculations were carried out using the TURBOMOLE program (Version 5.10, TURBOMOLE GmbH, Karlsruhe, see). For the computation of binding energies we employed the BP86 functional with a SV(P) basis set and an empirical disperison correction.
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    • The Kohn-Sham UP spectrum is given by the energy differences εLUMO - εi +IP, where εi are the orbital eigenvalues from a DFT calculation [BP86/SV(P)] of the cation at the geometry of the neutral and IP is the corresponding ionization potential. This is a good approximation to a UP spectrum where the dominant states are those resulting from removal of one electron, with no further excitation. For comparison with experiment, the spectra shown in Fig. 5c and 5d were shifted by 5.0 and 5.3 eV, respectively, and the Gaussian line width was chosen to give the UP peak profiles (FWHM=0.34 eV). The best fit of the experimental spectrum has been obtained after expanding the theoretical energy scale by 9%.
    • The Kohn-Sham UP spectrum is given by the energy differences εLUMO-εi +IP, where εi are the orbital eigenvalues from a DFT calculation [BP86/SV(P)] of the cation at the geometry of the neutral and IP is the corresponding ionization potential. This is a good approximation to a UP spectrum where the dominant states are those resulting from removal of one electron, with no further excitation. For comparison with experiment, the spectra shown in Fig. 5c and 5d were shifted by 5.0 and 5.3 eV, respectively, and the Gaussian line width was chosen to give the UP peak profiles (FWHM=0.34 eV). The best fit of the experimental spectrum has been obtained after expanding the theoretical energy scale by 9%.
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    • Footnote: A significant portion of the incident kinetic energy component can be converted into surface parallel motion (see Ref. 38).
    • Footnote: A significant portion of the incident kinetic energy component can be converted into surface parallel motion (see Ref. 38).


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