The electronic structure as well as the optical response of kesterite and stannite structures of Cu2ZnSnS4 and Cu 2ZnSnSe4 are analyzed by a relativistic full-potential linearized augmented plane wave method. The energy dispersion of the conduction-band edge reveals larger effective electron mass of the two Cu 2ZnSnS4 compounds (mc1 ≈0.18 m0) compared with Cu2ZnSnSe4 (mc1 ≈0.07 m 0). Whereas the effective electron mass tensor is fairly isotropic, the effective hole masses show strong anisotropy. The fundamental band-gap energy is estimated to be Eg ≈1.5 eV for Cu2ZnSnS 4 and Eg ≈1.0 eV for Cu2ZnSnSe4. The larger band gap results in a smaller high-frequency dielectric constant: ε∞ ≈6.7 for Cu2ZnSnS4 whereas ε∞ ≈8.6 for Cu2ZnSnSe4. The characteristic anisotropy of the dielectric function ε (ω) in the stannite compounds allows for a complementary identification of the crystalline structure type. Overall, however, all four compounds show similar atomic-resolved density-of-states, dielectric function, and optical absorption coefficient α (ω). © 2010 American Institute of Physics.
CITATION STYLE
Persson, C. (2010). Electronic and optical properties of Cu2ZnSnS4 and Cu2ZnSnSe4. Journal of Applied Physics, 107(5). https://doi.org/10.1063/1.3318468
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