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Energy Procedia 60 (2014) 43 – 47 Available online at www.sciencedirect.com ScienceDirect 1876-6102 © 2014 The Authors. Published by Elsevier Ltd. This is an open access article under the CC BY-NC-ND license (http://creativecommons.org/licenses/by-nc-nd/3.0/). Peer-review under responsibility of The European Materials Research Society (E-MRS) doi:10.1016/j.egypro.2014.12.340 E-MRS Spring Meeting 2014 Symposium Y “Advanced materials and characterization techniques for solar cells II, 26-30 May 2014, Lille, France Effects of the morphology of chemically deposited Zn(O,S) buffer layers on the performance Cu(In,Ga)Se 2 solar cell. Tetsuhito Okamoto a *, Hironori Komaki b , Junji Sasano a , Shigeru Niki b , Masanobu Izaki a a Toyohashi Univercity of Technology, 1-1 Hibarigaoka, Tenpaku-cho, Toyohashi, Aichi 441-8122, Japan b National Institute of Advanced Industrial Science and Technology(AIST), 1-1-1 Umezono, Tukuba, Ibaraki 305-8568, Japan Abstract Zinc sulfide oxide Zn(O,S) buffer layers were prepared by a chemical bath deposition (CBD) method, and the effects of the deposition time on the structure and performance of the Cu(In,Ga)Se 2 (CIGS) solar cells were investigated by structural, optical and electrical characterizations. The CBD deposition time affected the thickness and morphology of the Zn(O,S) layer, and the thickness and surface roughness decreased by decreasing the deposition time. The conversion efficiency of 15.5% has been obtained for the CIGS solar cells with the Zn(O,S) buffer layer prepared under optimized condition. Keywords: Zn(O,S), Cu(In,Ga)Se2, buffer layer, CBD method, deposition condition ; 1. Introduction Cu(In,Ga)Se 2 (CIGS) solar cell composed of n-ZnO(window layer)/buffer layer/CIGS/Mo electrode is a thin film solar cell which has been already put to practical use because of the high efficiency and low cost. The use of CdS installed into the conventional CIGS solar cell is limited because of the environmental problem and small band gap, * Corresponding author. Tel.: +0-000-000-0000 E-mail address: [email protected] © 2014 The Authors. Published by Elsevier Ltd. This is an open access article under the CC BY-NC-ND license (http://creativecommons.org/licenses/by-nc-nd/3.0/). Peer-review under responsibility of The European Materials Research Society (E-MRS)

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  • Energy Procedia 60 ( 2014 ) 43 – 47

    Available online at www.sciencedirect.com

    ScienceDirect

    1876-6102 © 2014 The Authors. Published by Elsevier Ltd. This is an open access article under the CC BY-NC-ND license (http://creativecommons.org/licenses/by-nc-nd/3.0/).Peer-review under responsibility of The European Materials Research Society (E-MRS)doi: 10.1016/j.egypro.2014.12.340

    E-MRS Spring Meeting 2014 Symposium Y “Advanced materials and characterization techniques for solar cells II”, 26-30 May 2014, Lille, France

    Effects of the morphology of chemically deposited Zn(O,S) buffer layers on the performance Cu(In,Ga)Se2 solar cell.

    Tetsuhito Okamotoa*, Hironori Komakib, Junji Sasanoa, Shigeru Nikib, Masanobu Izakia aToyohashi Univercity of Technology, 1-1 Hibarigaoka, Tenpaku-cho, Toyohashi, Aichi 441-8122, Japan

    bNational Institute of Advanced Industrial Science and Technology(AIST), 1-1-1 Umezono, Tukuba, Ibaraki 305-8568, Japan

    Abstract

    Zinc sulfide oxide Zn(O,S) buffer layers were prepared by a chemical bath deposition (CBD) method, and the effects of the deposition time on the structure and performance of the Cu(In,Ga)Se2 (CIGS) solar cells were investigated by structural, optical and electrical characterizations. The CBD deposition time affected the thickness and morphology of the Zn(O,S) layer, and the thickness and surface roughness decreased by decreasing the deposition time. The conversion efficiency of 15.5% has been obtained for the CIGS solar cells with the Zn(O,S) buffer layer prepared under optimized condition. © 2014 The Authors. Published by Elsevier Ltd. Peer-review under responsibility of the scientific committee of the SiliconPV 2014 conference.

    Keywords: Zn(O,S), Cu(In,Ga)Se2, buffer layer, CBD method, deposition condition ;

    1. Introduction

    Cu(In,Ga)Se2 (CIGS) solar cell composed of n-ZnO(window layer)/buffer layer/CIGS/Mo electrode is a thin film solar cell which has been already put to practical use because of the high efficiency and low cost. The use of CdS installed into the conventional CIGS solar cell is limited because of the environmental problem and small band gap,

    * Corresponding author. Tel.: +0-000-000-0000

    E-mail address: [email protected]

    © 2014 The Authors. Published by Elsevier Ltd. This is an open access article under the CC BY-NC-ND license (http://creativecommons.org/licenses/by-nc-nd/3.0/).Peer-review under responsibility of The European Materials Research Society (E-MRS)

    http://crossmark.crossref.org/dialog/?doi=10.1016/j.egypro.2014.12.340&domain=pdfhttp://crossmark.crossref.org/dialog/?doi=10.1016/j.egypro.2014.12.340&domain=pdf

  • 44 Tetsuhito Okamoto et al. / Energy Procedia 60 ( 2014 ) 43 – 47

    which leads to decrease in photoelectric conversion efficiency. The Zn(O,S) is a realistic candidate of the buffer layer alternative to the CdS due to the optical and electrical characteristics, shown by [1].

    The Zn(O,S) buffer layer was formed by chemical bath deposition (CBD) method used for the CdS formation. The Zn(O,S) buffer layer which was mixture of zinc oxide (ZnO), zinc sulfide (ZnS) and zinc hydroxide (Zn(OH)2) shown by [2], and was composed of the upper Zn(OH)2 and lower crystalline Zn(O,S) layers. The upper Zn(OH)2 acts as the obstacle for transporting carrier generated in CIGS layer because of the large conduction band offset researched by [3]. We have decreased a etching process with the dipped in ammonia (NH3) water to remove the upper zinc hydroxide layer (NH3 etching process). The removal of the upper zinc hydroxide layer by NH3 etching process resulted in the improvement of the conversion efficiency of the CIGS cell using Zn(O,S) from 6.75% to 13.7%. Since, the conversion efficiency was lower than that with CdS buffer, further optimization of the preparation condition is needed for the improvement of the further conversion efficiency.

    In this study, the CBD method used for fabricating the Zn(O,S) buffer layer was optimized based on the structural and morphological characterization. And, the CIGS solar cell was fabricated using the Zn(O,S) buffer layer, and the photovoltaic performance was under AM. 1.5 G illumination.

    2. Experimental

    2.1. Preparation of the Zn(O,S) buffer layer by CBD and the deposition

    The Zn(O,S) buffer layer were formed on CIGS/Mo/soda lime glass (SLG) substrate by the CBD process. The CIGS layer was prepared on a Mo-coated glass substrate (3 cm × 3 cm in size) by a 3 stage vapor deposition system. The composition of the CBD solution was 1.5 mol/L NH3 water, 0.1 mol/L zinc nitrate, and 0.4 mol/L thiourea. The CIGS substrate was immersed into the CBD solution and then heated at 80 degrees C with stirring 300 rpm. The deposition time was varied from 10 to 17 minutes (min), and other conditions were fixed. The conversion efficiencies of 13.67% was already obtained for the Zn(O,S) layer deposited 17 min. After the CBD deposition, the NH3 etching process was carried out by sample. Fig.1 shows NH3 etching process. The samples were rinsed with pure water and dipped into a alkali aqueous solution containing 0.5 mol/L NH3,for 10 seconds.

    The Zn(O,S) layer was analyzed by field emission scanning electron microscope (FE-SEM), atomic force microscope (AFM) and x-ray photoelectron spectroscopy (XPS) to estimate the film thickness, surface roughness, and surface composition.

    2.2. Construction of CIGS solar cell

    After the buffer layer process, CIGS solar cell devices were fabricated by stacking the i-ZnO as a high-resistivity layer, Al-doped ZnO window (ZnO:Al) layer, and Al electrode. The i-ZnO and ZnO:Al layers were deposited by a RF magnetron sputtering, and an Al layer was deposited on the top by a vapor deposition.

    After the preparing of the CIGS device, the conversion efficiency was estimated by recording the current-voltage curve under simulated AM1.5 G illumination.

    Fig. 1 The CBD process for preparing Zn(O,S) buffer layer on CIGS/Mo substrate

  • Tetsuhito Okamoto et al. / Energy Procedia 60 ( 2014 ) 43 – 47 45

    Fig. 2 FE-SEM images of cross-sectioned structure of CIGS/Mo/SLG substrate with Zn(O,S) layer deposition time of (a)10 and (b)17 min

    3. Results and discussion

    3.1. Film thickness of Zn(O,S) layers

    Fig. 2 shows cross-sectional FE-SEM images of Zn(O,S)-10min/CIGS absorber/Mo electrode and Zn(O,S)-17min/CIGS/Mo. The surface roughness of the Zn(O,S) buffer layer at 10 min was homogenous in comparison with the 17 min. The thickness of the Zn(O,S) layer was estimate to be approximately 150 and 200 nm from the images. The Zn(O,S) buffer layer thickness was decreased by shorting the CBD deposition time. The decrease in the thickness of the Zn(O,S) layer affects the series resistance of the resultant CIGS solar cell, because of the high resistivity.

    3.2. Surface roughness of Zn(O,S) layers

    Fig. 3 shows the topography images of the CIGS surface before and after the Zn(O,S) layer deposition for 10 and 17 min. Large number of particles identifier as Zn(O,S) grains could be observed on the surface. Size of the grain was estimated to be about 80 and 60 nm at 17 min for 10 min. The surface roughness with arithmetic mean estimation (Ra) was estimated to be 46.22 μm for 10 min and 54.87 μm for 17 min, and 50.76 μm was obtained for the bare CIGS. The decrease in the deposition time induced the improvement of the surface roughness.

    Fig. 3. Topography images of CIGS before(c) and after the deposition of Zn(O,S) layers deposited for (a)10 and (b)17min

    b a c

    a b

    bbbb c

    b

  • 46 Tetsuhito Okamoto et al. / Energy Procedia 60 ( 2014 ) 43 – 47

    3.3. Composition of Zn(O,S) buffer layer

    Fig. 4 shows the electron narrow spectra of Zn 2p3/2, O 1s, and S 2p3/2. The peak at 1022eV was observed on the Zn2p electron spectrum and could be identified as that of Zn2+ ion ZnO and Zn(OH)2. The O1s electron spectra showed a peak energy at binding energy of 530 eV, which identified as O2- in ZnO, and small shoulder could be observed at around 531.2 eV originated from OH- ion Zn(OH)2. The intensity of the OH- shorder decreased with decrease in the deposition time, indicating the decrease in the OH- content. The peak of S2- in ZnS could be observed at around 162 eV, in addition to peaks identified as Se in CIGS. The S2- peak decreased with decrease in the deposition time.

    The concentration of Zn, O, and S was estimated with the sensitivity factor, and the 10-min-deposited Zn(O,S) layer was composed of 15.03%-Zn(OH)2, 41.50%-ZnO, and 43.47%-ZnS and 17-min-deposited Zn(O,S) layer was composed of 23.86%-Zn(OH)2, 35.39%-ZnO, and 40.75%-ZnS, respectively. The content of Zn(OH)2, ZnO, and ZnS. The Zn(OH)2 content decreased with the decrease in the deposition time. It was already reported that the Zn(OH)2 had a harmful effect on the photovoltaic characteristics of the CIGS solar cell.

    3.4. The performance of CIGS solar cells with Zn(O,S) layers

    Fig. 5 shows current-voltage curves of CIGS solar cells with Zn(O,S) layers at deposition time of 10 and 17 min. The conversion efficiency of CIGS solar cell was improved from 6.75 to 13.67 % by removing the upper zinc hydroxide layer. The CIGS solar cell with Zn(O,S) buffer layer deposited at 17 min showed the conversion efficiency of 13.67 % with Voc = 0.64 V, Jsc = 33.4 mA/cm2, and FF = 0.64. The shortening the deposition time to 10 min induced the improvement of the conversion efficiency to 15.50% with Voc = 0.65V, Jsc = 34.1 mA/cm2 and FF = 0.70. The improvement indicated the conformal formation of the Zn(O,S) layer at 10 min, and the conversion efficiency was improved by the decrease in the thickness, surface roughness and Zn(OH)2 content.

    Fig. 4 The electron spectra for Zn(O,S) layers deposited on CIGS substrate at (a) 10 and (b) 17 min.

    a b c

  • Tetsuhito Okamoto et al. / Energy Procedia 60 ( 2014 ) 43 – 47 47

    Fig. 5 Current density - voltage curves for CIGS solar cells with Zn(O,S) layers deposited for 10 and 17 min. Non-etching represented the CIGS

    with Zn(O,S) layer without NH3 etching.

    4. Conclution

    Zn(O,S) buffer layers were prepared by a chemical bath deposition (CBD) method, and the effects of the deposition time on the structure and performance of the Cu(In,Ga)Se2 (CIGS) solar cells were investigated by structural, and electrical characterizations with FE-SEM, AFM, and XPS. The decrease in the deposition time included the decrease in the film thickness, surface, toughness, and Zn(OH)2 content. The convention efficiency was improved from 13.7% to 15.5% by decrease the deposition time from 17 to 10 min. The results demonstrated here indicated the importance of the morphological and structural characteristics of the Zn(O,S) layer on the CIGS solar cell performance.

    Acknowledgements

    This work was supported by the New Energy and Industrial Technology Development Organization. (NEDO)

    References

    [1] C. Hubert, N. Nag havi, B. Canava, A.Etcheberry, D.Lincot, Thin Solid Films, 515(2007), 6032-6035. [2] B. Mokili, Y.Charreire, R. Cortes, D. Lincot, Thin Solid Films, 288 (1996)21-28, [3] N. Terada, R.T.Widodo, K. Itoh, S.H.kong, H.Kashiwabara, T.Okuda, K.Obara, S.Niki, K.Sakurai, A.Yamada, S.Ishizuka, Thin Solid Films,

    480-481 (2005), 183

    Zn(O,S)-10min Zn(O,S)-

    17min Non-etching

    Voc (V) 0.650 0.639 0.538

    Jsc (mA/cm2) 34.0 33.4 25.6

    FF 0.699 0.640 0.490

    Eff (%) 15.5 13.7 6.75

    Zn(O,S)-10min Zn(O,S)-17min

    Non-etching