The crystal structure of silver is body-centred cubic (Figure 4.4a), and so the Ag(111) plane exhibits a close-packed, hexagonal structure (Figure 4.4b). Ag is a stable transition metal, and one of the few metals found abundantly in nature as a pure native element. This stability is due to its relative inertness, and the Ag(111) close-packed surface has the lowest energy of its high-symmetry surfaces.
As discussed in Section 4.2, molecules on Ag(111) tend to favour close-packed arrangements where possible. Its low surface energy allows molecules to easily diffuse until they encounter either a step edge (with a higher energy due to symmetry breaking), or another molecule (with whom the intermolecular interaction is stronger than the molecule–substrate interaction), giving rise to close-packed monolayers. The surface is not completely ignored by the deposited molecules however, with the choice of substrate playing a major role in the properties of NiDPP and MnClTPP (Chapter 5).
Ag/Si(111)- × R30° consists of the honeycomb-chain trimer structure. Cleaving the (111) surface of Si creates dangling bonds that point out of the surface into the vacuum. If it is not passivated, these bonds reconstruct into chains of dimers, however when Ag is deposited onto the Si(111) surface, it forms pseudo-hexagons on the surface, which cause the Si dangling bonds to reconstruct into trimers [187–189], as shown in Figure 4.5.
The Ag/Si(111)- × R30° surface was chosen as its reactivity is expected to be intermediate in strength between that of clean Si(111) and hydrogen-passivated Si(111) [190, 191]. On clean Si(111), porphyrin molecules form covalent bonds and are unable to diffuse or self-assemble into ordered structures at room temperature [161, 181], while on the H-passivated surface they diffuse freely and can form islands [181, 192]. The effect of the Ag(111) surface on the NiDPP self-assembly is expected to be minor, similar to that of H-passivated Si(111), however the Ag/Si(111)- × R30° surface’s electron states have been shown to exhibit a resonance close to the energy of the dz2 molecular orbital , leading to a stronger interaction with the surface, and the difference between the interactions with these two surfaces will be explored in this chapter.