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. 2016 Jan 2;138(3):1010–1016. doi: 10.1021/jacs.5b12124

Figure 3.

Figure 3

(A) Absorption and PL spectra of CsPbBr3 as a thin film (see Figure SI13), cube-shaped nanocrystals, and NPLs of different thicknesses. (B) Employed cubic CsPbBr3 2D slabs and unit supercell. a–b are the periodic dimensions. (C) Comparison of the experimental (green line) and SR- and SOC-DFT calculated band gaps (black line and red line, respectively) as a function of the NPLs inverse squared dimension (1/r2).