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. 2017 Nov 15;9(3):735–742. doi: 10.1039/c7sc04312k

Fig. 3. Selected BP/SV(P) (continuum solvent model for DCM) optimized low-energy structures of H6DPP (left) and H6(DPP)2 (right). ΔE and nB values are, respectively, relative energies (in kcal mol–1) and the corresponding Boltzmann populations (in %, at 25 °C); in parentheses are data for calculations without the solvent model.

Fig. 3