4.6 Article

A study of ternary Cu2SnS3 and Cu3SnS4 thin films prepared by sulfurizing stacked metal precursors

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IOP PUBLISHING LTD
DOI: 10.1088/0022-3727/43/21/215403

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  1. Fundacao para a Ciencia e Tecnologia (FCT) [SFRH/BD/49220/2008, SFRH/BD/29881/2006]
  2. National Electronic Microscopy Network [REDE/1509/RME/2005]
  3. Fundação para a Ciência e a Tecnologia [SFRH/BD/29881/2006] Funding Source: FCT

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Thin films of Cu2SnS3 and Cu3SnS4 were grown by sulfurization of dc magnetron sputtered Sn-Cu metallic precursors in a S-2 atmosphere. Different maximum sulfurization temperatures were tested which allowed the study of the Cu2SnS3 phase changes. For a temperature of 350 degrees C the films were composed of tetragonal (I-42m) Cu2SnS3. The films sulfurized at a maximum temperature of 400 degrees C presented a cubic (F-43m) Cu2SnS3 phase. On increasing the temperature up to 520 degrees C, the Sn content of the layer decreased and orthorhombic (Pmn21) Cu3SnS4 was formed. The phase identification and structural analysis were performed using x-ray diffraction (XRD) and electron backscattered diffraction (EBSD) analysis. Raman scattering analysis was also performed and a comparison with XRD and EBSD data allowed the assignment of peaks at 336 and 351 cm(-1) for tetragonal Cu2SnS3, 303 and 355 cm(-1) for cubic Cu2SnS3, and 318, 348 and 295 cm(-1) for the Cu3SnS4 phase. Compositional analysis was done using energy dispersive spectroscopy and induced coupled plasma analysis. Scanning electron microscopy was used to study the morphology of the layers. Transmittance and reflectance measurements permitted the estimation of absorbance and band gap. These ternary compounds present a high absorbance value close to 104 cm(-1). The estimated band gap energy was 1.35 eV for tetragonal (I-42m) Cu2SnS3, 0.96 eV for cubic (F-43m) Cu2SnS3 and 1.60 eV for orthorhombic (Pmn21) Cu3SnS4. A hot point probe was used for the determination of semiconductor conductivity type. The results show that all the samples are p-type semiconductors. A four-point probe was used to obtain the resistivity of these samples. The resistivities for tetragonal Cu2SnS3, cubic Cu2SnS3 and orthorhombic (Pmn21) Cu3SnS4 are 4.59 x 10(-2) Omega cm, 1.26 x 10(-2) Omega cm, 7.40 x 10(-4) Omega cm, respectively.

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