Phys Rev B 49:7697–7708ĭubois SM, Lopez-Bezanilla A, Cresti A, Triozon F, Biel B, Charlier JC, Roche S (2010) Quantum transport in graphene nanoribbons: effects of edge reconstruction and chemical reactivity. Tamura R, Tsukada M (1994) Disclinations of monolayer graphite and their electronic states. Energy Environ Sci 5:8848–8868Īn B, Fukuyama S, Yokogawa K, Yoshimura M, Egashira M, Korai Y, Mochida I (2001) Single pentagon in a hexagonal carbon lattice revealed by scanning tunneling microscopy. Huang C, Li C, Shi G (2012) Graphene based catalysts. Proposed FWHMs can be adjusted by measuring actual FWHMs using each device. Based on the calculated and the actual results, we proposed peak shifts and FWHMs of graphene with the different number of pentagons, which can be utilized for analyzing actual XPS spectra. These calculated shifts and FWHMs were close to the actual shifts of graphite (284.0 eV) and fullerene (282.9 eV) and FWHMs of graphite (1.25 eV) and fullerene (1.15 eV). The FWHM reached at 1.15 eV by introducing twelve pentagons (fullerene). Introduction of six pentagons increased the calculated FWHMs from 1.25 to 1.45 eV, whereas introduction of eight or more pentagons decreased the FWHMs. The presence of pentagons also influenced FWHMs. Introduction of up to four isolated pentagons had no influence on shifts of the calculated peak maxima of graphene (284.0 eV), whereas the introduction of six or more pentagons shifted the calculated peak maximum toward low binding energies because the number of connected pentagons increased.
#Urethane c1s xps peak full
Peak shifts and full width at half maximum (FWHM) of calculated C1s spectra were compared with those of actual C1s spectra. C1s X-ray photoelectron spectroscopy (XPS) spectra of graphene with two to eight pentagons and fullerene pentagons were simulated using density functional theory calculation.
0 kommentar(er)
