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Beilstein J. Nanotechnol. 2017, 8, 1723–1733, doi:10.3762/bjnano.8.173
Figure 1: Mass spectra recorded at a) different gas pressures (5, 10, 15 and 20 mTorr) and at different power...
Figure 2: a) Evolution of the normalized ion signals, extracted from the mass spectra at different plasma pow...
Figure 3: C 1s and F 1s core level spectra acquired from fluorinated vCNT after plasma treatments at differen...
Figure 4: Representative Raman spectra of pristine and fluorinated vCNT (a). Evolution of intensity (I) and a...
Figure 5: (a) Valence band spectra acquired from pristine (black line) and fluorinated vCNT with different fl...
Figure 6: The stability of the fluorination is presented as a function of time for four different samples con...
Beilstein J. Nanotechnol. 2015, 6, 2242–2251, doi:10.3762/bjnano.6.230
Figure 1: Top views (a), (b) and side views (c), (d) of bridge (B) and top (T) sites, respectively, where (a)...
Figure 2: (a,b) Side views of the isodensity plot showing the bond charge of pentacene at the B-site for an i...
Figure 3: Comparison between the Kohn–Sham eigenvalues of the V-shaped gas phase pentacene with coordinates e...
Figure 4: Experimental C 1s XPS spectrum for pentacene/Al(001) compared with the simulated spectra of (a) fre...
Figure 5: Top and side views of the screening charges in the presence of a full core hole on (a,b,c) C1 at th...
Figure 6: Simulated NEXAFS of the gas phase V-shaped pentacene from the B-site along the z-direction of the f...
Figure 7: (a) Analysis of the initial state effects in the simulated NEXAFS spectrum and its comparison with ...