High Temperature Annealing of ZnO:Al on Passivating POLO Junctions: Impact on Transparency, Conductivity, Junction Passivation, and Interface Stability

Research output: Contribution to journalArticleResearchpeer review

Authors

  • Tobias F. Wietler
  • Byungsul Min
  • Sina Reiter
  • Yevgeniya Larionova
  • Rolf Reineke-Koch
  • Frank Heinemeyer
  • Rolf Brendel
  • Armin Feldhoff
  • Jan Krugener
  • Dominic Tetzlaff
  • Robby Peibst

External Research Organisations

  • Technische Universität Braunschweig
  • Institute for Solar Energy Research (ISFH)
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Details

Original languageEnglish
Article number8565997
Pages (from-to)89-96
Number of pages8
JournalIEEE journal of photovoltaics
Volume9
Issue number1
Publication statusPublished - Jan 2019

Abstract

We investigate the enhancement in transparency and conductivity of aluminum doped zinc oxide (ZnO:Al) layers upon high-Temperature annealing and its impact on contact resistance, as well as, on passivation properties of carrier selective junctions based on doped polycrystalline Si on a passivating silicon oxide (POLO). The temperature stability of these junctions allows annealing of the ZnO:Al/POLO combination up to 600 °C. We prepare ZnO:Al films by dc magnetron sputtering at room temperature. We determine the complex refractive index of ZnO:Al in dependence of post-deposition annealing (PDA) temperature by spectroscopic ellipsometry. High-Temperature annealing improves the conductivity and reduces the absorption within ZnO:Al. The optical losses in a ZnO:Al/POLO stack are rather limited by the poly-Si layer than by the ZnO:Al. The sheet resistance improves from roughly 20000 Ω/sq for 80 nm thick as-deposited ZnO:Al films to 72 Ω/sq after fast firing at 600 °C. At the same time, PDA cures the damage induced in the POLO junctions during ZnO:Al deposition. After PDA with AlxOy capping layers, the passivation quality even surpasses the initial level. A transmission electron microscopy analysis of the interface between the ZnO:Al and the underlying poly-Si reveals the formation of a silicon oxide like interfacial layer after PDA at 400 °C. This interfacial layer causes a high contact resistivity of the metal/ZnO:Al/POLO-junction and could limit the thermal budget for cell processing. Our results indicate that after successful process adjustment, ZnO:Al could substitute In-based transparent conductive oxides on POLO cells for cost reasons, as well as, enable a high efficiency potential.

Keywords

    Passivating contacts, POLO junction, polycrystalline silicon, thermal treatment, ZnO:Al

ASJC Scopus subject areas

Cite this

High Temperature Annealing of ZnO:Al on Passivating POLO Junctions: Impact on Transparency, Conductivity, Junction Passivation, and Interface Stability. / Wietler, Tobias F.; Min, Byungsul; Reiter, Sina et al.
In: IEEE journal of photovoltaics, Vol. 9, No. 1, 8565997, 01.2019, p. 89-96.

Research output: Contribution to journalArticleResearchpeer review

Wietler, T. F., Min, B., Reiter, S., Larionova, Y., Reineke-Koch, R., Heinemeyer, F., Brendel, R., Feldhoff, A., Krugener, J., Tetzlaff, D., & Peibst, R. (2019). High Temperature Annealing of ZnO:Al on Passivating POLO Junctions: Impact on Transparency, Conductivity, Junction Passivation, and Interface Stability. IEEE journal of photovoltaics, 9(1), 89-96. Article 8565997. https://doi.org/10.1109/JPHOTOV.2018.2878337
Wietler TF, Min B, Reiter S, Larionova Y, Reineke-Koch R, Heinemeyer F et al. High Temperature Annealing of ZnO:Al on Passivating POLO Junctions: Impact on Transparency, Conductivity, Junction Passivation, and Interface Stability. IEEE journal of photovoltaics. 2019 Jan;9(1):89-96. 8565997. doi: 10.1109/JPHOTOV.2018.2878337
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title = "High Temperature Annealing of ZnO:Al on Passivating POLO Junctions: Impact on Transparency, Conductivity, Junction Passivation, and Interface Stability",
abstract = "We investigate the enhancement in transparency and conductivity of aluminum doped zinc oxide (ZnO:Al) layers upon high-Temperature annealing and its impact on contact resistance, as well as, on passivation properties of carrier selective junctions based on doped polycrystalline Si on a passivating silicon oxide (POLO). The temperature stability of these junctions allows annealing of the ZnO:Al/POLO combination up to 600 °C. We prepare ZnO:Al films by dc magnetron sputtering at room temperature. We determine the complex refractive index of ZnO:Al in dependence of post-deposition annealing (PDA) temperature by spectroscopic ellipsometry. High-Temperature annealing improves the conductivity and reduces the absorption within ZnO:Al. The optical losses in a ZnO:Al/POLO stack are rather limited by the poly-Si layer than by the ZnO:Al. The sheet resistance improves from roughly 20000 Ω/sq for 80 nm thick as-deposited ZnO:Al films to 72 Ω/sq after fast firing at 600 °C. At the same time, PDA cures the damage induced in the POLO junctions during ZnO:Al deposition. After PDA with AlxOy capping layers, the passivation quality even surpasses the initial level. A transmission electron microscopy analysis of the interface between the ZnO:Al and the underlying poly-Si reveals the formation of a silicon oxide like interfacial layer after PDA at 400 °C. This interfacial layer causes a high contact resistivity of the metal/ZnO:Al/POLO-junction and could limit the thermal budget for cell processing. Our results indicate that after successful process adjustment, ZnO:Al could substitute In-based transparent conductive oxides on POLO cells for cost reasons, as well as, enable a high efficiency potential.",
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note = "Funding information: December 21, 2018. This work was supported in part by the Ministry for Science tablished concept to realize such junctions is the application of andCultureofLowerSaxony,theGermanMinistryforEconomicAffairsand heterojunctions using surface passivating intrinsic and doped Horizon2020researchandinnovationprogramunderGrant727529(DISC).EnergyunderGrant0325702(POLO)andinpartbytheEuropeanUnion{\textquoteright}s hydrogenated amorphous silicon (a-Si:H) layers on the front (Corresponding author: Tobias F. Wietler.) and rear side of the solar cell [2], [3]. An alternative also with T.F.Wietler,B.Min,S.Reiter,Y.Larionova,R.Reineke-Koch,F.Heine- excellent interface passivation quality is the junction between merthal31860,Germany(e-mail:,wietler@isfh.de;min@isfh.de;reiter@isfh.meyerarewiththeInstituteforSolarEnergyResearchHamelin(ISFH),Em- crystalline (c-) and polycrystalline (poly-) silicon with an em-de; larionova@isfh.de; r.reineke-koch@isfh.de; heinemeyer@isfh.de). bedded interfacial silicon oxide (POLO) [4], [5]. Very low re-R.BrendeliswiththeInstituteforSolidStatePhysics,LeibnizUniversita¨t combination current densities enable a conversion efficiency of ergyResearchHamelin(ISFH),Emmerthal31860,Germany(e-mail:,brendel@Hannover,Hanover30167,Germany,andalsowiththeInstituteforSolarEn- 26.1% for a POLO-cell with interdigitated back contacts [6]. isfh.de). Over a wide range of the spectrum, doped poly-Si has a lower J.Kru¨generiswiththeInstituteofElectronicMaterialsandDevices(MBE), absorption coefficient than doped a-Si:H, implying a signifi-A.Feldhoff is withtheInstituteforPhysical Chemistryand Electro-Hanover30167,Germany(e-mail:,kruegener@mbe.uni-hannover.de). cantly lower absorption loss in a poly-Si layer than in an a-Si:H chemistry, Leibniz Universit{\"a}t Hannover, Hanover 30167, Germany (e-mail:, layer with the same thickness [7]–[9]. For a 15 nm thick, doped armin.feldhoff@pci.uni-hannover.de). poly-Si layer, for example, the parasitic absorption induces a sita¨tBraunschweig,Braunschweig38106,Germany(e-mail:,dominic.tetzlaff@D.Tetzlaff is withthe Instituteof AppliedPhysics,Technische Univer- loss in the short-circuit current density of 0.75 mA/cm2. For a tu-braunschweig.de). doped a-Si:H layer with the same thickness, the corresponding R.PeibstiswiththeInstituteforSolarEnergyResearchHamelin(ISFH), loss is 3 mA/cm2 [7]. However, less than 20 nm thin poly-Si andDevices(MBE),Hanover30167,Germany(e-mail:,peibst@isfh.de).Emmerthal31860,Germany,andalsowiththeInstituteofElectronicMaterials layers have sheet resistances above 1000 ?/sq [10]. A highly This paper has supplementary downloadable material available at conductive and transparent layer on top of the poly-Si could help http://ieeexplore.ieee.orgprovidedbytheauthor. to ensure the required lateral conductivity for the transport of athttp://ieeexplore.ieee.org.Colorversionsofoneormoreofthefiguresinthispaperareavailableonline charge carriers toward the metallization grid on the front side. German Ministry for Economic Affairs and Energy under Grant 0325702",
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Download

TY - JOUR

T1 - High Temperature Annealing of ZnO:Al on Passivating POLO Junctions

T2 - Impact on Transparency, Conductivity, Junction Passivation, and Interface Stability

AU - Wietler, Tobias F.

AU - Min, Byungsul

AU - Reiter, Sina

AU - Larionova, Yevgeniya

AU - Reineke-Koch, Rolf

AU - Heinemeyer, Frank

AU - Brendel, Rolf

AU - Feldhoff, Armin

AU - Krugener, Jan

AU - Tetzlaff, Dominic

AU - Peibst, Robby

N1 - Funding information: December 21, 2018. This work was supported in part by the Ministry for Science tablished concept to realize such junctions is the application of andCultureofLowerSaxony,theGermanMinistryforEconomicAffairsand heterojunctions using surface passivating intrinsic and doped Horizon2020researchandinnovationprogramunderGrant727529(DISC).EnergyunderGrant0325702(POLO)andinpartbytheEuropeanUnion’s hydrogenated amorphous silicon (a-Si:H) layers on the front (Corresponding author: Tobias F. Wietler.) and rear side of the solar cell [2], [3]. An alternative also with T.F.Wietler,B.Min,S.Reiter,Y.Larionova,R.Reineke-Koch,F.Heine- excellent interface passivation quality is the junction between merthal31860,Germany(e-mail:,wietler@isfh.de;min@isfh.de;reiter@isfh.meyerarewiththeInstituteforSolarEnergyResearchHamelin(ISFH),Em- crystalline (c-) and polycrystalline (poly-) silicon with an em-de; larionova@isfh.de; r.reineke-koch@isfh.de; heinemeyer@isfh.de). bedded interfacial silicon oxide (POLO) [4], [5]. Very low re-R.BrendeliswiththeInstituteforSolidStatePhysics,LeibnizUniversita¨t combination current densities enable a conversion efficiency of ergyResearchHamelin(ISFH),Emmerthal31860,Germany(e-mail:,brendel@Hannover,Hanover30167,Germany,andalsowiththeInstituteforSolarEn- 26.1% for a POLO-cell with interdigitated back contacts [6]. isfh.de). Over a wide range of the spectrum, doped poly-Si has a lower J.Kru¨generiswiththeInstituteofElectronicMaterialsandDevices(MBE), absorption coefficient than doped a-Si:H, implying a signifi-A.Feldhoff is withtheInstituteforPhysical Chemistryand Electro-Hanover30167,Germany(e-mail:,kruegener@mbe.uni-hannover.de). cantly lower absorption loss in a poly-Si layer than in an a-Si:H chemistry, Leibniz Universität Hannover, Hanover 30167, Germany (e-mail:, layer with the same thickness [7]–[9]. For a 15 nm thick, doped armin.feldhoff@pci.uni-hannover.de). poly-Si layer, for example, the parasitic absorption induces a sita¨tBraunschweig,Braunschweig38106,Germany(e-mail:,dominic.tetzlaff@D.Tetzlaff is withthe Instituteof AppliedPhysics,Technische Univer- loss in the short-circuit current density of 0.75 mA/cm2. For a tu-braunschweig.de). doped a-Si:H layer with the same thickness, the corresponding R.PeibstiswiththeInstituteforSolarEnergyResearchHamelin(ISFH), loss is 3 mA/cm2 [7]. However, less than 20 nm thin poly-Si andDevices(MBE),Hanover30167,Germany(e-mail:,peibst@isfh.de).Emmerthal31860,Germany,andalsowiththeInstituteofElectronicMaterials layers have sheet resistances above 1000 ?/sq [10]. A highly This paper has supplementary downloadable material available at conductive and transparent layer on top of the poly-Si could help http://ieeexplore.ieee.orgprovidedbytheauthor. to ensure the required lateral conductivity for the transport of athttp://ieeexplore.ieee.org.Colorversionsofoneormoreofthefiguresinthispaperareavailableonline charge carriers toward the metallization grid on the front side. German Ministry for Economic Affairs and Energy under Grant 0325702

PY - 2019/1

Y1 - 2019/1

N2 - We investigate the enhancement in transparency and conductivity of aluminum doped zinc oxide (ZnO:Al) layers upon high-Temperature annealing and its impact on contact resistance, as well as, on passivation properties of carrier selective junctions based on doped polycrystalline Si on a passivating silicon oxide (POLO). The temperature stability of these junctions allows annealing of the ZnO:Al/POLO combination up to 600 °C. We prepare ZnO:Al films by dc magnetron sputtering at room temperature. We determine the complex refractive index of ZnO:Al in dependence of post-deposition annealing (PDA) temperature by spectroscopic ellipsometry. High-Temperature annealing improves the conductivity and reduces the absorption within ZnO:Al. The optical losses in a ZnO:Al/POLO stack are rather limited by the poly-Si layer than by the ZnO:Al. The sheet resistance improves from roughly 20000 Ω/sq for 80 nm thick as-deposited ZnO:Al films to 72 Ω/sq after fast firing at 600 °C. At the same time, PDA cures the damage induced in the POLO junctions during ZnO:Al deposition. After PDA with AlxOy capping layers, the passivation quality even surpasses the initial level. A transmission electron microscopy analysis of the interface between the ZnO:Al and the underlying poly-Si reveals the formation of a silicon oxide like interfacial layer after PDA at 400 °C. This interfacial layer causes a high contact resistivity of the metal/ZnO:Al/POLO-junction and could limit the thermal budget for cell processing. Our results indicate that after successful process adjustment, ZnO:Al could substitute In-based transparent conductive oxides on POLO cells for cost reasons, as well as, enable a high efficiency potential.

AB - We investigate the enhancement in transparency and conductivity of aluminum doped zinc oxide (ZnO:Al) layers upon high-Temperature annealing and its impact on contact resistance, as well as, on passivation properties of carrier selective junctions based on doped polycrystalline Si on a passivating silicon oxide (POLO). The temperature stability of these junctions allows annealing of the ZnO:Al/POLO combination up to 600 °C. We prepare ZnO:Al films by dc magnetron sputtering at room temperature. We determine the complex refractive index of ZnO:Al in dependence of post-deposition annealing (PDA) temperature by spectroscopic ellipsometry. High-Temperature annealing improves the conductivity and reduces the absorption within ZnO:Al. The optical losses in a ZnO:Al/POLO stack are rather limited by the poly-Si layer than by the ZnO:Al. The sheet resistance improves from roughly 20000 Ω/sq for 80 nm thick as-deposited ZnO:Al films to 72 Ω/sq after fast firing at 600 °C. At the same time, PDA cures the damage induced in the POLO junctions during ZnO:Al deposition. After PDA with AlxOy capping layers, the passivation quality even surpasses the initial level. A transmission electron microscopy analysis of the interface between the ZnO:Al and the underlying poly-Si reveals the formation of a silicon oxide like interfacial layer after PDA at 400 °C. This interfacial layer causes a high contact resistivity of the metal/ZnO:Al/POLO-junction and could limit the thermal budget for cell processing. Our results indicate that after successful process adjustment, ZnO:Al could substitute In-based transparent conductive oxides on POLO cells for cost reasons, as well as, enable a high efficiency potential.

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