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Vibrational signatures of OTe and OTe–VCd in CdTe: A first-principles study AITranslate

Kasetsart University; Suranaree University of Technology and Synchrotron Light Research Institute; University of California; University of California;Oak Ridge National Laboratory;Oak Ridge National Laboratory;Oak Ridge National Laboratory
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Publisher: Elsevier
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Abstract AITranslate

Chen et al. [Phys. Rev. Lett. 96 (2006) 035508] experimentally observed vibrational signatures related to defects in oxygen-doped CdTe using ultrahigh resolution Fourier transform infrared (FTIR) spectroscopy. They observed an absorption peak at 350 cm−1. In addition, for samples grown under certain conditions, they observed two higher frequency peaks (1097 and 1108 cm−1) at low temperature that merged into one at room-temperature. They attributed the low-frequency peak (350 cm−1) to the vibration of OTe and the two higher frequency peaks to the vibrational modes of a OTe–VCd complex. Subsequently, they reported similar modes around 1100 cm−1 in O-doped CdSe [Phys. Rev. Lett. 101 (2008) 195502] which were attributed to an OSe–VCd complex. We employed first-principles DFT calculations to calculate the vibrational modes of OTe and OTe–VCd complex in CdTe. Our calculations show that the 350 cm−1 mode is consistent with OTe. However, the frequencies of the modes around 1100 cm−1 are more than twice the expected frequencies for OTe–VCd complexes in CdTe (or OSe–VCd in CdSe), indicating that the OTe–VCd complex cannot be the cause of the observed 1100 cm−1 modes. A search for a new defect model is in order.

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DOI:https://doi.org/10.1016/j.commatsci.2010.01.024

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Chen et al. [Phys. Rev. Lett. 96 (2006) 035508] experimentally observed vibrational signatures related to defects in oxygen-doped CdTe using ultrahigh resolution Fourier transform infrared (FTIR) spectroscopy. They observed an absorption peak at 350 cm−1. In addition, for samples grown under certain conditions, they observed two higher frequency peaks (1097 and 1108 cm−1) at low temperature that merged into one at room-temperature. They attributed the low-frequency peak (350 cm−1) to the vibration of OTe and the two higher frequency peaks to the vibrational modes of a OTe–VCd complex. Subsequently, they reported similar modes around 1100 cm−1 in O-doped CdSe [Phys. Rev. Lett. 101 (2008) 195502] which were attributed to an OSe–VCd complex. We employed first-principles DFT calculations to calculate the vibrational modes of OTe and OTe–VCd complex in CdTe. Our calculations show that the 350 cm−1 mode is consistent with OTe. However, the frequencies of the modes around 1100 cm−1 are more than twice the expected frequencies for OTe–VCd complexes in CdTe (or OSe–VCd in CdSe), indicating that the OTe–VCd complex cannot be the cause of the observed 1100 cm−1 modes. A search for a new defect model is in order.

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GB/T 7714-2015 [1] J. TThienprasert, S. Limpijumnong, A. Janotti, et al. Computational Materials Science, 2010(49). DOI:10.1016/j.commatsci.2010.01.024.
MLA [1] J. TThienprasert, et al., Computational Materials Science, no. 49, 2010, https://doi.org/10.1016/j.commatsci.2010.01.024.
APA [1] J. TThienprasert, S. Limpijumnong, A. Janotti, C.G. Van de Walle, L. Zhang, M.H. Du, & D.J. Singh. (2010). Computational Materials Science(49). https://doi.org/10.1016/j.commatsci.2010.01.024
IEEE [1] J. TThienprasert, S. Limpijumnong, A. Janotti, C.G. Van de Walle, L. Zhang, M.H. Du, and D.J. Singh, Computational Materials Science, no. 49, 2010, doi: 10.1016/j.commatsci.2010.01.024.