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crushing 26amp 3b screening theory in pdf

explicitly shown in Fig. 3B (black dots). The reason is that conduction and valence band profiles are almost unaffected by P(Fig. 2), as the band edges are displaced in k space, which prevents the macroscopic dielectric constant from diverging (red dots in Fig. 3B). Were the closing gap direct, metal-like screening would dissociate the exciton.

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