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. 2021 Aug 13;9:734076. doi: 10.3389/fchem.2021.734076

FIGURE 1.

FIGURE 1

Photophysical properties of ht-PLPPAN (A) Experimental and simulated UV-vis spectra of ht-PLPPAN calculated by time-dependent density functional theory (TDDFT). Structure optimization and TDDFT calculations were performed in simulated water environment using a polarizable continuum model, at the ωB97X-D/6-31g-d and cam-b3lyp/6-31g-d levels, respectively (B) A representative model structure for photoactive domains of ht-PLPPAN with four nitrogen atoms (oI4), optimized at the ωB97X-D/6-31g-d level (Stephens et al., 1994; Frisch et al., 2016). (C) Energy levels of the lowest unoccupied molecular orbital (LUMO, black bars) and wavelengths of the lowest energy transition (red squares) of model structures (oI3 to oI10) with different conjugation lengths represented by the number of nitrogen atoms within the backbone (Sun et al., 2020). The dashed line represents the energy of the LUMO (β) of the [Br-CuII/TPMA]+ complex in water [optimized at the ωB97X-D level with def2TZVP basis set on Cu and 6-31g-d basis set on the other atoms (Miertuš and Tomasi, 1981; Chai and Head-Gordon, 2008)].