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Tin monosulfide (SnS) was grown by atomic layer deposition (ALD) using sequential exposures of tin(II) 2,4-
pentanedionate (Sn(acac)2) and hydrogen sulfide (H2S). In situ quartz crystal microbalance (QCM) studies showed that
the SnS ALD mass gain per cycle was 11-12 ng/cm2 at 175°C on a gold-covered QCM sensor. Using a film density of
5.07 g/cm3 determined by X-ray reflectivity measurements, these mass gains are equivalent to SnS ALD growth rates of
0.22-0.24 Å/cycle. The ratio of the mass loss and mass gain ratio |▵m2/▵m1| from the H2S and Sn(acac)2 reactions was
|▵m2/▵m1| ~0.32 at 175 °C. This measured ratio is close to the predicted ratio from the proposed surface chemistry for
SnS ALD. The SnS ALD was self-limiting versus the Sn(acac)2 and H2S exposures. The SnS ALD growth rate was also
independent of substrate temperature from 125-225 °C. X-ray fluorescence studies confirmed a Sn/S atomic ratio of
~1.0 for the SnS ALD films. X-ray photoelectron spectroscopy measurements revealed that the SnS ALD films
contained oxygen impurities at 15-20 at% after air exposure. These oxygen-containing SnS ALD films displayed a
bandgap of ~1.87 eV that is higher than the SnS bulk value of ~1.3 eV.
Jay Yu Kim andSteven M. George
"Tin monosulfide thin films grown by atomic layer deposition using tin 2,4 pentandionate and hydrogen sulfide", Proc. SPIE 7769, High and Low Concentrator Systems for Solar Electric Applications V, 776907 (24 August 2010); https://doi.org/10.1117/12.855890
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Jay Yu Kim, Steven M. George, "Tin monosulfide thin films grown by atomic layer deposition using tin 2,4 pentandionate and hydrogen sulfide," Proc. SPIE 7769, High and Low Concentrator Systems for Solar Electric Applications V, 776907 (24 August 2010); https://doi.org/10.1117/12.855890