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Documento PDF - UniCA Eprints - Università degli studi di Cagliari.

Documento PDF - UniCA Eprints - Università degli studi di Cagliari.

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3.3 adhesion of a single p3ht molecule on the zinc oxide surface 33Figure 3.2.: Trench grooves (T.G.) and row of <strong>di</strong>mers (R.D.) in a portionof ZnO.scale model after atomic relaxation based on MPMD is reporte<strong>di</strong>n Figure 3.2 The atomic scale structure of the (10¯10)surface exhibit trench grooves alternated with rows of ZnO<strong>di</strong>mers (channels), both oriented along the [010] crystallographic<strong>di</strong>rection. Hereafter in this chapter, the x axis isalways chosen parallel to this [010] crystallographic <strong>di</strong>rectionFigure 3.2. As already <strong>di</strong>scussed in chapter 1, in orderto describe the ZnO crystalline surface, we adopt theBuckingham-type potential. This potential describes properlyseveral properties of bulk and nanocrystals such aselastic constants, equilibrium lattice energy, cell parameters,elastic and <strong>di</strong>electric constants [72].3.3 adhesion of a single p3ht molecule on thezinc oxide surfaceThe first step in the analysis of the ZnO/P3HT interfaceis the study of the adhesion of a single polymer moleculeon the surface. For this purpose a P3HT molecule composedby 16 monomers is put at <strong>di</strong>fferent <strong>di</strong>stances fromthe surface with the thiophene rings parallel to it (face-onalignment) and the backbone parallel to the ZnO <strong>di</strong>mers.The basin of interaction between the ZnO and the P3HTis reported in Figure 3.3, where the unrelaxed energy (calculatedwithout allowing atomic relaxation of the polymerdue to the surface) is reported as a function of the relative<strong>di</strong>stance between molecule and surface. The minimumof the interaction is found at 3.7 Å and corresponds to

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