1 research outputs found
Cu(In,Ga)Se<sub>2</sub> Solar Cells with Amorphous In<sub>2</sub>O<sub>3</sub>‑Based Front Contact Layers
Amorphous (<i>a</i>-) In<sub>2</sub>O<sub>3</sub>-based front contact layers composed of transparent
conducting oxide (TCO) and transparent oxide semiconductor (TOS) layers
were proved to be effective in enhancing the short-circuit current
density (<i>J</i><sub>sc</sub>) of CuÂ(In,Ga)ÂSe<sub>2</sub> (CIGS) solar cells with a glass/Mo/CIGS/CdS/TOS/TCO structure, while
maintaining high fill factor (FF) and open-circuit voltage (<i>V</i><sub>oc</sub>). An <i>n</i>-type <i>a</i>-In–Ga–Zn–O layer was introduced between the
CdS and TCO layers. Unlike unintentionally doped ZnO broadly used
as TOS layers in CIGS solar cells, the grain-boundaryÂ(GB)-free amorphous
structure of the <i>a</i>-In–Ga–Zn–O
layers allowed high electron mobility with superior control over the
carrier density (<i>N</i>). High FF and <i>V</i><sub>oc</sub> values were achieved in solar cells containing <i>a</i>-In–Ga–Zn–O layers with <i>N</i> values broadly ranging from 2 × 10<sup>15</sup> to 3 ×
10<sup>18</sup> cm<sup>–3</sup>. The decrease in FF and <i>V</i><sub>oc</sub> produced by the electronic inhomogeneity
of solar cells was mitigated by controlling the series resistance
within the TOS layer of CIGS solar cells. In addition, <i>a</i>-In<sub>2</sub>O<sub>3</sub>:H and <i>a-</i>In–Zn–O
layers exhibited higher electron mobilities than the ZnO:Al layers
conventionally used as TCO layers in CIGS solar cells. The In<sub>2</sub>O<sub>3</sub>-based layers exhibited lower free carrier absorption
while maintaining similar sheet resistance than ZnO:Al. The TCO and
TOS materials and their combinations did not significantly change
the <i>V</i><sub>oc</sub> of the CIGS solar cells and the
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