2018
DOI: 10.1021/acs.jpcc.8b08945
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High-Resolution Near-Edge X-ray Absorption Fine Structure Study of Condensed Polyacenes

Abstract: We present a systematic study of high-resolution NEXAFS spectra of well-ordered films of condensed benzene and polyacenes, namely naphthalene, anthracene, tetracene, and pentacene. An increased spectral complexity with increasing molecular size is observed: NEXAFS features decrease in intensity and moves to lower photon energy (redshift), as the size of the aromatic system grows. Moreover, a second group of transitions arises. The dichroism in the C K-edge spectra increases with the molecular size. While benze… Show more

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Cited by 9 publications
(14 citation statements)
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“…Figure c) shows nicely that the lowest energy excitations of the different perfluorinated acenes (indicated by dashed lines), which correspond to excitations into the LUMO, decrease with the acene length, as indicated by the calculated orbital energies (cf. Figure ) and parallels the situation observed for the nonsubstituted acenes . A precise assignment of the other π* resonances is not so simple, as initial state effects (i.e., slight differences in the C 1s binding energy for the different carbon atoms within the molecule), as well as final state effects, such as electron relaxation also affect the NEXAFS spectra.…”
Section: Resultssupporting
confidence: 60%
“…Figure c) shows nicely that the lowest energy excitations of the different perfluorinated acenes (indicated by dashed lines), which correspond to excitations into the LUMO, decrease with the acene length, as indicated by the calculated orbital energies (cf. Figure ) and parallels the situation observed for the nonsubstituted acenes . A precise assignment of the other π* resonances is not so simple, as initial state effects (i.e., slight differences in the C 1s binding energy for the different carbon atoms within the molecule), as well as final state effects, such as electron relaxation also affect the NEXAFS spectra.…”
Section: Resultssupporting
confidence: 60%
“…The split resonances located at 284.6 and 285.3 eV can be assigned to CC (C 1s→π*) from chemically different carbons. [ 64 ] The similar peak located at 285.5 eV in the spectrum of SA‐Fe/CN shows only one peak because the N‐doped graphite substrate possesses inequivalent carbons with a continuous chemical state, indicating the carbonization of Fe(phen) 3 . The peak located at 288.5 eV is attributed to C 1s→π* of CN in the spectra of both samples.…”
Section: Resultsmentioning
confidence: 99%
“…The split resonances located at 284.6 and 285.3 eV can be assigned to CC (C 1s→π*) from chemically different carbons. [64] The similar peak located at 285.5 eV in the spectrum of SA-Fe/CN shows only one peak because the N-doped graphite substrate possesses inequivalent Adv. Mater.…”
Section: Synthesis and Characterization Of Sa-fe/cnmentioning
confidence: 99%
“…Following earlier reports on 6A (and also 5A ), the lowest lying main features in C 1s XAS spectra (photon energies <288 eV, denoted A–D in Figure 5 ), can be attributed to transitions into π* orbitals. 12 , 74 , 77 , 78 …”
Section: Resultsmentioning
confidence: 99%