Examination of electronic structure differences between CIGSSe and CZTSSe by photoluminescence study
In this paper, we elaborate on the interpretation and use of photoluminescence (PL) measurements as they relate to the “donor/acceptor” and “electrostatic potential fluctuations” models for compensated semiconductors. Low-temperature (7 K) PL measurements were performed on high-efficiency Cu(In,Ga)(...
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sg-ntu-dr.10356-1042502023-02-28T19:44:58Z Examination of electronic structure differences between CIGSSe and CZTSSe by photoluminescence study Tai, Kong Fai Gershon, Talia Gunawan, Oki Huan, Cheng Hon Alfred School of Physical and Mathematical Sciences Photons Thin film devices Blue shift Photoluminescence Band gap In this paper, we elaborate on the interpretation and use of photoluminescence (PL) measurements as they relate to the “donor/acceptor” and “electrostatic potential fluctuations” models for compensated semiconductors. Low-temperature (7 K) PL measurements were performed on high-efficiency Cu(In,Ga)(S,Se)2 and two Cu2ZnSn(S,Se)4 solar cells with high- and low-S/(S + Se) ratio, all fabricated by a hydrazine solution-processing method. From excitation-dependent PL, the total defect density (which include radiative and non-radiative defects) within the band gap (Eg) was estimated for each material and the consequent depth of the electrostatic potential fluctuation (γ) was calculated. The quasi-donor-acceptor pair (QDAP) density was estimated from the blue-shift magnitude of the QDAP PL peak position in power-dependent PL spectra. As a further verification, we show that the slope of the lifetime as a function of photon energies (dτ/dE) is consistent with our estimate for the magnitude of γ. Lastly, the energetic depth of the QDAP defects is examined by studying the spectral evolution of the PL as a function of temperature. The shallow defect levels in CIGSSe resulted in a significant blue-shift of the PL peak with temperature, whereas no obvious shift was observed for either CZTSSe sample, indicating an increase in the depth of the defects. Further improvement on Cu2ZnSn(S,Se)4 solar cell should focus on reducing the sub-Eg defect density and avoiding the formation of deep defects. Published version 2015-10-16T06:01:25Z 2019-12-06T21:29:03Z 2015-10-16T06:01:25Z 2019-12-06T21:29:03Z 2015 2015 Journal Article Tai, K. F., Gershon, T., Gunawan, O., & Huan, C. H. A. (2015). Examination of electronic structure differences between CIGSSe and CZTSSe by photoluminescence study. Journal of Applied Physics, 117(23), 235701-. https://hdl.handle.net/10356/104250 http://hdl.handle.net/10220/38808 10.1063/1.4922493 en Journal of Applied Physics © 2015 American Institute of Physics (AIP). This paper was published in Journal of Applied Physics and is made available as an electronic reprint (preprint) with permission of American Institute of Physics (AIP). The published version is available at: [http://dx.doi.org/10.1063/1.4922493]. One print or electronic copy may be made for personal use only. Systematic or multiple reproduction, distribution to multiple locations via electronic or other means, duplication of any material in this paper for a fee or for commercial purposes, or modification of the content of the paper is prohibited and is subject to penalties under law. application/pdf |
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Photons Thin film devices Blue shift Photoluminescence Band gap Tai, Kong Fai Gershon, Talia Gunawan, Oki Huan, Cheng Hon Alfred Examination of electronic structure differences between CIGSSe and CZTSSe by photoluminescence study |
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In this paper, we elaborate on the interpretation and use of photoluminescence (PL) measurements as they relate to the “donor/acceptor” and “electrostatic potential fluctuations” models for compensated semiconductors. Low-temperature (7 K) PL measurements were performed on high-efficiency Cu(In,Ga)(S,Se)2 and two Cu2ZnSn(S,Se)4 solar cells with high- and low-S/(S + Se) ratio, all fabricated by a hydrazine solution-processing method. From excitation-dependent PL, the total defect density (which include radiative and non-radiative defects) within the band gap (Eg) was estimated for each material and the consequent depth of the electrostatic potential fluctuation (γ) was calculated. The quasi-donor-acceptor pair (QDAP) density was estimated from the blue-shift magnitude of the QDAP PL peak position in power-dependent PL spectra. As a further verification, we show that the slope of the lifetime as a function of photon energies (dτ/dE) is consistent with our estimate for the magnitude of γ. Lastly, the energetic depth of the QDAP defects is examined by studying the spectral evolution of the PL as a function of temperature. The shallow defect levels in CIGSSe resulted in a significant blue-shift of the PL peak with temperature, whereas no obvious shift was observed for either CZTSSe sample, indicating an increase in the depth of the defects. Further improvement on Cu2ZnSn(S,Se)4 solar cell should focus on reducing the sub-Eg defect density and avoiding the formation of deep defects. |
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School of Physical and Mathematical Sciences |
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School of Physical and Mathematical Sciences Tai, Kong Fai Gershon, Talia Gunawan, Oki Huan, Cheng Hon Alfred |
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Article |
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Tai, Kong Fai Gershon, Talia Gunawan, Oki Huan, Cheng Hon Alfred |
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Tai, Kong Fai |
title |
Examination of electronic structure differences between CIGSSe and CZTSSe by photoluminescence study |
title_short |
Examination of electronic structure differences between CIGSSe and CZTSSe by photoluminescence study |
title_full |
Examination of electronic structure differences between CIGSSe and CZTSSe by photoluminescence study |
title_fullStr |
Examination of electronic structure differences between CIGSSe and CZTSSe by photoluminescence study |
title_full_unstemmed |
Examination of electronic structure differences between CIGSSe and CZTSSe by photoluminescence study |
title_sort |
examination of electronic structure differences between cigsse and cztsse by photoluminescence study |
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2015 |
url |
https://hdl.handle.net/10356/104250 http://hdl.handle.net/10220/38808 |
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1759854918238208000 |