TY - JOUR
T1 - Dielectric function and double absorption onset of monoclinic Cu2SnS3
T2 - Origin of experimental features explained by first-principles calculations
AU - Crovetto, Andrea
AU - Chen, Rongzhen
AU - Ettlinger, Rebecca Bolt
AU - Cazzaniga, Andrea Carlo
AU - Schou, Jørgen
AU - Persson, Clas
AU - Hansen, Ole
PY - 2016
Y1 - 2016
N2 - In this work, we determine experimentally the dielectric function of monoclinic Cu2SnS3 (CTS) by spectroscopic ellipsometry from 0.7 to 5.9 eV. An experimental approach is proposed to overcome the challenges of extracting the dielectric function of Cu2SnS3 when grown on a glass/Mo substrate, as relevant for photovoltaic applications. The ellipsometry measurement reveals a double absorption onset at 0.91 eV and 0.99 eV. Importantly, we demonstrate that calculation within the density functional theory (DFT) confirms this double onset only when a very dense k-mesh is used to reveal fine details in the electronic structure, and this can explain why it has not been reported in earlier calculated spectra. We can now show that the double onset originates from optical transitions at the Γ-point from three energetically close-lying valence bands to a single conduction band. Thus, structural imperfection, like secondary phases, is not needed to explain such an absorption spectrum. Finally, we show that the absorption coefficient of CTS is particularly large in the near-band gap spectral region when compared to similar photovoltaic materials.
AB - In this work, we determine experimentally the dielectric function of monoclinic Cu2SnS3 (CTS) by spectroscopic ellipsometry from 0.7 to 5.9 eV. An experimental approach is proposed to overcome the challenges of extracting the dielectric function of Cu2SnS3 when grown on a glass/Mo substrate, as relevant for photovoltaic applications. The ellipsometry measurement reveals a double absorption onset at 0.91 eV and 0.99 eV. Importantly, we demonstrate that calculation within the density functional theory (DFT) confirms this double onset only when a very dense k-mesh is used to reveal fine details in the electronic structure, and this can explain why it has not been reported in earlier calculated spectra. We can now show that the double onset originates from optical transitions at the Γ-point from three energetically close-lying valence bands to a single conduction band. Thus, structural imperfection, like secondary phases, is not needed to explain such an absorption spectrum. Finally, we show that the absorption coefficient of CTS is particularly large in the near-band gap spectral region when compared to similar photovoltaic materials.
KW - CTS
KW - Cu2SnS3
KW - Optical properties
KW - Band gap
KW - Ellipsometry
U2 - 10.1016/j.solmat.2016.04.028
DO - 10.1016/j.solmat.2016.04.028
M3 - Journal article
SN - 0927-0248
VL - 154
SP - 121
EP - 129
JO - Solar Energy Materials & Solar Cells
JF - Solar Energy Materials & Solar Cells
ER -