Growth of amorphous Zn–Sn–O thin films by RF sputtering for buffer layers of CuInSe2 and SnS solar cells
We propose using amorphous Zn–Sn–O (α-ZTO) deposited by RF sputtering as an alternative n-type buffer layer for Cu(In,Ga)Se2 and SnS solar cells. The order of the carrier density, n, is increased from the order of 1015 to 1017cm−1 as the Sn/(Sn+Zn) atomic ratio increases from 0.29 to 0.40. On the ot...
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Veröffentlicht in: | Thin solid films 2015-08, Vol.589, p.408-411 |
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Sprache: | eng |
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Zusammenfassung: | We propose using amorphous Zn–Sn–O (α-ZTO) deposited by RF sputtering as an alternative n-type buffer layer for Cu(In,Ga)Se2 and SnS solar cells. The order of the carrier density, n, is increased from the order of 1015 to 1017cm−1 as the Sn/(Sn+Zn) atomic ratio increases from 0.29 to 0.40. On the other hand, the order of n decreased from 1017 to 1011cm−1 as the oxygen partial pressure increased from 0 to 10%. Further, for the α-ZTO film with the Sn/(Sn+Zn) atomic ratio at 0.38 and the oxygen partial pressure at 0%, valence band discontinuities of α-ZTO/CuInSe2 and α-ZTO/SnS were determined using photoelectron yield spectroscopy measurements. The band discontinuities of each of these interfaces form a spike structure in the conduction band offset, which enables a high-performance solar cell to be obtained.
•We propose using amorphous Zn–Sn–O as a n-type layer for Cu(In,Ga)Se2 and SnS solar cells.•The carrier density was controlled by total and/or oxygen partial pressure during sputtering.•Valence band discontinuities of Zn–Sn–O/CuInSe2 and Zn–Sn–O/SnS were determined.•The conduction band discontinuities of each of these interfaces form a spike structure. |
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ISSN: | 0040-6090 1879-2731 |
DOI: | 10.1016/j.tsf.2015.06.003 |