Abstract
The geometrical and electronic properties of the monolayer (ML) of tetracene (Tc) molecules on Ag(111) are systematically investigated by means of DFT calculations with the use of localized basis set. The bridge and hollow adsorption positions of the molecule in the commensurate $\gamma$-Tc/Ag(111) are revealed to be the most stable and equally favorable irrespective to the approximation chosen for the exchange-correlation functional. The binding energy is entirely determined by the long-range dispersive interaction. The former lowest unoccupied orbital remains being unoccupied in the case of $\gamma$-Tc/Ag(111) as well as in the $\alpha$-phase with increased coverage. The unit cell of the $\alpha$-phase with point-on-line registry was adapted for calculations based on the available experimental data and the computed structures of the $\gamma$-phase. The calculated position of the Tc/Ag(111) interface state is found to be noticeably dependent on the lattice constant of the substrate, however its energy shift with respect to the Shockley surface state of the unperturbed clean side of the slab is sensitive only to the adsorption distance and in good agreement with the experimentally measured energy shift.
Highlights
Organic molecular thin films are currently of great interest because of their possible applications in micro- and optoelectronic devices[1,2]
Because of the obvious disadvantage of the Γ1 geometry, it will excluded from our further analysis, but despite the unfavorable adsorption structure of Γ0, it will be considered as a reference structure proposed by experimentalists[24]
We performed the theoretical study of the Tc/Ag(111) metal-organic interface by means of density functional theory (DFT) calculations with localized basis
Summary
Organic molecular thin films are currently of great interest because of their possible applications in micro- and optoelectronic devices[1,2]. The presence of interface electronic states (ISs)[7,8,9] is an additional agent influencing the overall charge transfer, albeit role of these states in the process and the mechanism of their formation are not yet fully understood[10]. On one hand, such hybrid states can be formed as the result of the chemical interaction of molecular orbitals with metallic states[7,11,12,13]. The lateral corrugation of the IS local density of states above the metal substrate resembles that of organic molecular orbitals[9,14,15,16,18,19]
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