Department of Chemistry2024-11-0920101432-881X10.1007/s00214-009-0661-62-s2.0-77957684773http://dx.doi.org/10.1007/s00214-009-0661-6https://hdl.handle.net/20.500.14288/12937The interaction potential energy of triphenylene dimer has been calculated with Møller–Plesset second-order perturbation theory for various geometrical configurations. Different types of geometrical perturbations such as rotation, displacements and their combinations are studied in terms of their effects on the stability of the dimer. Minimum energy conformers for face to face, rotated, parallel displaced and T-shape structures are obtained. For the unsubstituted triphenylene, the 35° rotation of one of the monomers results in the global minimum. However, the dimer is still very flexible in terms of displacements. A helical structure seems to be the most stable form for the trimer. For large stacked clusters, the two body forces dominate the interactions while at small monomer–monomer separation, three body terms behave like z −9 where z is the vertical distance between two adjacent monomers.Chemistry, physical and theoreticalJournal Article282508000004Q49915