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Interfacial barrier height modification of indium tin oxide/a-Si:H(p) via control of density of interstitial oxygen for silicon heterojunction solar cell application

An indium tin oxide (ITO) film with low carrier concentration (n), high mobility (μ) and high work function (ΦITO) is a beneficial material for the front electrode in heterojunction silicon (HJ) solar cells due to its low free-carrier absorption in the near-infrared wavelength and low Schottky barri...

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Published in:Thin solid films 2013-11, Vol.546, p.342-346
Main Authors: Ahn, Shihyun, Kim, Sunbo, Dao, Vinh Ai, Lee, Seungho, Iftiquar, S.M., Kim, Doyoung, Hussain, Shahzada Qamar, Park, Hyeongsik, Lee, Jaehyeong, Lee, Youngseok, Cho, Jaehyun, Kim, Sangho, Yi, Junsin
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creator Ahn, Shihyun
Kim, Sunbo
Dao, Vinh Ai
Lee, Seungho
Iftiquar, S.M.
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Lee, Jaehyeong
Lee, Youngseok
Cho, Jaehyun
Kim, Sangho
Yi, Junsin
description An indium tin oxide (ITO) film with low carrier concentration (n), high mobility (μ) and high work function (ΦITO) is a beneficial material for the front electrode in heterojunction silicon (HJ) solar cells due to its low free-carrier absorption in the near-infrared wavelength and low Schottky barrier height at the ITO/emitter-layer front contact. This low free-carrier absorption as well as the low Schottky barrier height increase the open-circuit voltage (Voc) and the short-circuit current density (Jsc), which in turn increases the overall cell efficiency (η). Hence, ITO films with lower n, higher μ and higher ΦITO were prepared by controlling the density of the interstitial oxygen [Oi] in the films and used as anti-reflection electrodes in HJ solar cells. With increasing [Oi] in the ITO, the preferential orientation of the (222) crystalline plane became more dominant. The ΦITO and μ increased from 4.87eV and 38.9 cm2V−1s−1 to 5.04eV and 48.79 cm2V−1s−1, respectively, whereas n decreased from 4.7×1020cm−3 to 2.8×1020cm−3. We attribute these changes to the chemisorbed oxygen into the ITO films, while the decrease of n is due to the ability of interstitial oxygen to capture electron, and the increase of μ is due to the reduction in free-carrier scattering. These ITO films were used to fabricate HJ solar cells. As [Oi] in the ITO film increased, the device performance improved and the best cell performance was obtained with Voc of 714mV, Jsc 34.79mA/cm2 and η of 17.82%. By computer simulation, we found that the higher ΦITO and μ but lower n were responsible for the enhanced cell performance. The cell performance, however, deteriorated due to poor film properties when [Oi] exceeded concentration limit from 3.2×1020cm−3. •The carrier concentration (n) decreases with increasing interstitial oxygen ([Oi]).•The Hall mobility (μ) and the work function (ΦITO) increases with increasing ([Oi].•High μ and high ΦITO but low n is beneficial for cell performance.•The best cell performance was obtained as [Oi] of 3.2×1020cm−3.
doi_str_mv 10.1016/j.tsf.2013.05.132
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This low free-carrier absorption as well as the low Schottky barrier height increase the open-circuit voltage (Voc) and the short-circuit current density (Jsc), which in turn increases the overall cell efficiency (η). Hence, ITO films with lower n, higher μ and higher ΦITO were prepared by controlling the density of the interstitial oxygen [Oi] in the films and used as anti-reflection electrodes in HJ solar cells. With increasing [Oi] in the ITO, the preferential orientation of the (222) crystalline plane became more dominant. The ΦITO and μ increased from 4.87eV and 38.9 cm2V−1s−1 to 5.04eV and 48.79 cm2V−1s−1, respectively, whereas n decreased from 4.7×1020cm−3 to 2.8×1020cm−3. We attribute these changes to the chemisorbed oxygen into the ITO films, while the decrease of n is due to the ability of interstitial oxygen to capture electron, and the increase of μ is due to the reduction in free-carrier scattering. These ITO films were used to fabricate HJ solar cells. As [Oi] in the ITO film increased, the device performance improved and the best cell performance was obtained with Voc of 714mV, Jsc 34.79mA/cm2 and η of 17.82%. By computer simulation, we found that the higher ΦITO and μ but lower n were responsible for the enhanced cell performance. 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This low free-carrier absorption as well as the low Schottky barrier height increase the open-circuit voltage (Voc) and the short-circuit current density (Jsc), which in turn increases the overall cell efficiency (η). Hence, ITO films with lower n, higher μ and higher ΦITO were prepared by controlling the density of the interstitial oxygen [Oi] in the films and used as anti-reflection electrodes in HJ solar cells. With increasing [Oi] in the ITO, the preferential orientation of the (222) crystalline plane became more dominant. The ΦITO and μ increased from 4.87eV and 38.9 cm2V−1s−1 to 5.04eV and 48.79 cm2V−1s−1, respectively, whereas n decreased from 4.7×1020cm−3 to 2.8×1020cm−3. We attribute these changes to the chemisorbed oxygen into the ITO films, while the decrease of n is due to the ability of interstitial oxygen to capture electron, and the increase of μ is due to the reduction in free-carrier scattering. These ITO films were used to fabricate HJ solar cells. As [Oi] in the ITO film increased, the device performance improved and the best cell performance was obtained with Voc of 714mV, Jsc 34.79mA/cm2 and η of 17.82%. By computer simulation, we found that the higher ΦITO and μ but lower n were responsible for the enhanced cell performance. The cell performance, however, deteriorated due to poor film properties when [Oi] exceeded concentration limit from 3.2×1020cm−3. •The carrier concentration (n) decreases with increasing interstitial oxygen ([Oi]).•The Hall mobility (μ) and the work function (ΦITO) increases with increasing ([Oi].•High μ and high ΦITO but low n is beneficial for cell performance.•The best cell performance was obtained as [Oi] of 3.2×1020cm−3.</abstract><cop>Amsterdam</cop><pub>Elsevier B.V</pub><doi>10.1016/j.tsf.2013.05.132</doi><tpages>5</tpages></addata></record>
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subjects Applied sciences
Barriers
Condensed matter: electronic structure, electrical, magnetic, and optical properties
Condensed matter: structure, mechanical and thermal properties
Density
Electrodes
Electronic structure and electrical properties of surfaces, interfaces, thin films and low-dimensional structures
Energy
Exact sciences and technology
Free-carrier absorption
Heterojunction solar cells
Heterojunctions
Indium tin oxide
Interstitial oxygen density
Interstitials
Natural energy
Photovoltaic conversion
Physics
Silicon
Solar cells. Photoelectrochemical cells
Solar energy
Structure and morphology
thickness
Surface double layers, schottky barriers, and work functions
Surfaces and interfaces
thin films and whiskers (structure and nonelectronic properties)
Thin film structure and morphology
Work function
title Interfacial barrier height modification of indium tin oxide/a-Si:H(p) via control of density of interstitial oxygen for silicon heterojunction solar cell application
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