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Beilstein J. Nanotechnol. 2021, 12, 559–565, doi:10.3762/bjnano.12.46
Figure 1: (a.) Scheme of the experiment. (b.) Large-scale (200 × 125 nm2) constant-current (I = 20 pA, V = 3....
Figure 2: STM/AFM characterisation of a h-BN/Cu(111) Moiré superstructure. (a., b.) Constant-current topograp...
Figure 3: Work function variation between rim (red) and valley (blue) areas measured using (a.) dI/dV at cons...
Figure 4: Local stiffness of h-BN/Cu(111). (a.) Topography of an 8 × 8 nm2 h-BN/Cu(111) area corresponding to...
Beilstein J. Nanotechnol. 2017, 8, 1388–1395, doi:10.3762/bjnano.8.140
Figure 1: a) STM topography image of pentacene on h-BN (U = −1 V, I = 50 pA). b) Large-scale STM topography i...
Figure 2: STS of pentacene on h-BN/Rh(111) showing the resonances of the frontier molecular orbitals. The red...
Figure 3: Spatial mapping of the molecular orbitals of pentacene. a) At positive bias voltages (LUMO), b) ins...
Figure 4: Spatial mapping of the molecular orbitals of pentacene by employing an STM tip without (left) and w...
Figure 5: Hückel calculations of the frontier molecular orbitals (HOMO and LUMO) of pentacene in the gas phas...
Figure 6: Energy-level diagram depicting the relations between Ea, Ei, Φ and the energies measured in STS for...
Figure 7: STS measurements of pentacene on various decoupling layers (see legend). In the case of Au(111) and...
Figure 8: Experimentally determined energies for Ea (red circles) and Ei (black squares) of pentacene versus ...