The energy resolution that can be achieved in x-ray photoelectron spectroscopy experiments allows to disentangle the contribution arising from the presence of a large variety of surface atoms in non-equivalent configurations which manifests itself not only with the appearance of different spectral components, but also as unusual lineshape. In the present work, we show that the fit of the C 1s core level spectrum of graphene grown on Ir(1 1 1) realized using 200 peaks based on ab initio calculations, accounting for the non-equivalent C atoms in the moiré cell, does not improve the fit quality with respect to the use of a single component. On the contrary, the quantitative fit quality can be drastically increased by introducing a dependency of the Lorentzian width on the distance between C and Ir first-layer atoms. This result is associated to the different electronic properties, and in particular to the different density of states of the σ and π bands, of C atoms sitting on TOP (hills) or FCC (valleys) regions of graphene w
Information hidden behind a single peak in the C 1s spectrum of graphene on Ir(111)
Loi, FedericoMembro del Collaboration Group
;Baraldi, Alessandro
Conceptualization
2024-01-01
Abstract
The energy resolution that can be achieved in x-ray photoelectron spectroscopy experiments allows to disentangle the contribution arising from the presence of a large variety of surface atoms in non-equivalent configurations which manifests itself not only with the appearance of different spectral components, but also as unusual lineshape. In the present work, we show that the fit of the C 1s core level spectrum of graphene grown on Ir(1 1 1) realized using 200 peaks based on ab initio calculations, accounting for the non-equivalent C atoms in the moiré cell, does not improve the fit quality with respect to the use of a single component. On the contrary, the quantitative fit quality can be drastically increased by introducing a dependency of the Lorentzian width on the distance between C and Ir first-layer atoms. This result is associated to the different electronic properties, and in particular to the different density of states of the σ and π bands, of C atoms sitting on TOP (hills) or FCC (valleys) regions of graphene wFile | Dimensione | Formato | |
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C1s Gr_Ir(111) Appl_Surf_Sci.pdf
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