Anti-reflective microcrystalline silicon oxide p-layer for thin-film silicon solar cells on ZnO
As a result from the development of silicon thin-film solar cells that had been conducted at Applied Materials over the last few years, we present a new kind of microcrystalline silicon oxide (μc-SiOx:H) based p-layer for the application in amorphous/microcrystalline (a-Si:H/μc-Si:H) tandem solar ce...
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creator | Schwanitz, Konrad Klein, Stefan Stolley, Tobias Rohde, Martin Severin, Daniel Trassl, Roland |
description | As a result from the development of silicon thin-film solar cells that had been conducted at Applied Materials over the last few years, we present a new kind of microcrystalline silicon oxide (μc-SiOx:H) based p-layer for the application in amorphous/microcrystalline (a-Si:H/μc-Si:H) tandem solar cells on ZnO substrates. The refractive index of this p-layer can be adjusted in the range 2–3.5 and therefore serves as a refractive index matching layer between ZnO (n∼2) and silicon (n∼4). By applying such a layer the reflection of solar cells can be reduced to 3%. This results in a significant short circuit current increase in thin-film solar cells. As a follow up to the recently published results of large area thin film silicon modules by us [1,2], we describe in this paper in detail the material properties of this new silicon oxide p-layer, the optimization of electrical and optical properties in solar cells and also the impact on the light induced degradation of a-Si/μc-Si tandem junction cells.
► We reached reduction of the reflection of 2–3% with the silicon oxide p-layer. ► The absolute initial cell efficiency gain amounts 0.1% and the stable cell efficiency gain is 0.4%. ► The silicon oxide p-layer enhances the top cell current up to 0.3mA/cm². ► The relative efficiency loss by LID is 9.1–10.5%, whereas with the conventional p-layer it is 12.5%. ► stabilized module efficiencies of 10.1% on 1100× 1300mm2 glass substrates have been reached |
doi_str_mv | 10.1016/j.solmat.2012.06.003 |
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► We reached reduction of the reflection of 2–3% with the silicon oxide p-layer. ► The absolute initial cell efficiency gain amounts 0.1% and the stable cell efficiency gain is 0.4%. ► The silicon oxide p-layer enhances the top cell current up to 0.3mA/cm². ► The relative efficiency loss by LID is 9.1–10.5%, whereas with the conventional p-layer it is 12.5%. ► stabilized module efficiencies of 10.1% on 1100× 1300mm2 glass substrates have been reached</description><identifier>ISSN: 0927-0248</identifier><identifier>EISSN: 1879-3398</identifier><identifier>DOI: 10.1016/j.solmat.2012.06.003</identifier><language>eng</language><publisher>Amsterdam: Elsevier B.V</publisher><subject>a-Si:H/μc-Si:H tandem cells ; Applied sciences ; Direct energy conversion and energy accumulation ; Electrical engineering. Electrical power engineering ; Electrical power engineering ; Energy ; Exact sciences and technology ; Materials ; Natural energy ; PECVD ; Photoelectric conversion ; Photovoltaic cells ; Photovoltaic conversion ; Refractive index ; Refractivity ; Silicon ; Silicon oxide p-layer ; Silicon oxides ; Silicon substrates ; Solar cells ; Solar cells. Photoelectrochemical cells ; Solar energy ; Thin film solar cells ; Thin films ; Zinc oxide ; ZnO</subject><ispartof>Solar energy materials and solar cells, 2012-10, Vol.105, p.187-191</ispartof><rights>2012 Elsevier B.V.</rights><rights>2015 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c435t-b4def3f424afbe93b8231b1b0d54d45eb6482b89ef432a5a4ee3e63c50fb2943</citedby><cites>FETCH-LOGICAL-c435t-b4def3f424afbe93b8231b1b0d54d45eb6482b89ef432a5a4ee3e63c50fb2943</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://www.sciencedirect.com/science/article/pii/S0927024812002814$$EHTML$$P50$$Gelsevier$$H</linktohtml><link.rule.ids>314,776,780,3537,27901,27902,65306</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=26280409$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>Schwanitz, Konrad</creatorcontrib><creatorcontrib>Klein, Stefan</creatorcontrib><creatorcontrib>Stolley, Tobias</creatorcontrib><creatorcontrib>Rohde, Martin</creatorcontrib><creatorcontrib>Severin, Daniel</creatorcontrib><creatorcontrib>Trassl, Roland</creatorcontrib><title>Anti-reflective microcrystalline silicon oxide p-layer for thin-film silicon solar cells on ZnO</title><title>Solar energy materials and solar cells</title><description>As a result from the development of silicon thin-film solar cells that had been conducted at Applied Materials over the last few years, we present a new kind of microcrystalline silicon oxide (μc-SiOx:H) based p-layer for the application in amorphous/microcrystalline (a-Si:H/μc-Si:H) tandem solar cells on ZnO substrates. The refractive index of this p-layer can be adjusted in the range 2–3.5 and therefore serves as a refractive index matching layer between ZnO (n∼2) and silicon (n∼4). By applying such a layer the reflection of solar cells can be reduced to 3%. This results in a significant short circuit current increase in thin-film solar cells. As a follow up to the recently published results of large area thin film silicon modules by us [1,2], we describe in this paper in detail the material properties of this new silicon oxide p-layer, the optimization of electrical and optical properties in solar cells and also the impact on the light induced degradation of a-Si/μc-Si tandem junction cells.
► We reached reduction of the reflection of 2–3% with the silicon oxide p-layer. ► The absolute initial cell efficiency gain amounts 0.1% and the stable cell efficiency gain is 0.4%. ► The silicon oxide p-layer enhances the top cell current up to 0.3mA/cm². ► The relative efficiency loss by LID is 9.1–10.5%, whereas with the conventional p-layer it is 12.5%. ► stabilized module efficiencies of 10.1% on 1100× 1300mm2 glass substrates have been reached</description><subject>a-Si:H/μc-Si:H tandem cells</subject><subject>Applied sciences</subject><subject>Direct energy conversion and energy accumulation</subject><subject>Electrical engineering. Electrical power engineering</subject><subject>Electrical power engineering</subject><subject>Energy</subject><subject>Exact sciences and technology</subject><subject>Materials</subject><subject>Natural energy</subject><subject>PECVD</subject><subject>Photoelectric conversion</subject><subject>Photovoltaic cells</subject><subject>Photovoltaic conversion</subject><subject>Refractive index</subject><subject>Refractivity</subject><subject>Silicon</subject><subject>Silicon oxide p-layer</subject><subject>Silicon oxides</subject><subject>Silicon substrates</subject><subject>Solar cells</subject><subject>Solar cells. Photoelectrochemical cells</subject><subject>Solar energy</subject><subject>Thin film solar cells</subject><subject>Thin films</subject><subject>Zinc oxide</subject><subject>ZnO</subject><issn>0927-0248</issn><issn>1879-3398</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2012</creationdate><recordtype>article</recordtype><recordid>eNp9kLtqwzAUhkVpoWnaN-jgpdDF7tHFjrwUQugNAlkydRGyfEQVZDuVnNC8fRUSOnY6HPjO5f8IuadQUKDV06aIg-_0WDCgrICqAOAXZELlrM45r-UlmUDNZjkwIa_JTYwbAGAVFxOi5v3o8oDWoxndHrPOmTCYcIij9t71mEXnnRn6bPhxLWbb3OsDhswOIRu_XJ9b57s_Jr2hQ2bQ-5il9rNf3ZIrq33Eu3OdkvXry3rxni9Xbx-L-TI3gpdj3ogWLbeCCW0brHkjGacNbaAtRStKbCohWSNrtIIzXWqByLHipgTbsFrwKXk8rd2G4XuHcVSdi8c_dI_DLioKkjFasZlMqDihKWeMKbnaBtfpcEiQOupUG3XSqY46FVQq6UxjD-cLOhrtbdC9cfFvllVMgoA6cc8nDlPavcOgonHYG2xdSIpVO7j_D_0CFoKOpg</recordid><startdate>20121001</startdate><enddate>20121001</enddate><creator>Schwanitz, Konrad</creator><creator>Klein, Stefan</creator><creator>Stolley, Tobias</creator><creator>Rohde, Martin</creator><creator>Severin, Daniel</creator><creator>Trassl, Roland</creator><general>Elsevier B.V</general><general>Elsevier</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7SP</scope><scope>7SU</scope><scope>7TB</scope><scope>7U5</scope><scope>8FD</scope><scope>C1K</scope><scope>FR3</scope><scope>L7M</scope></search><sort><creationdate>20121001</creationdate><title>Anti-reflective microcrystalline silicon oxide p-layer for thin-film silicon solar cells on ZnO</title><author>Schwanitz, Konrad ; Klein, Stefan ; Stolley, Tobias ; Rohde, Martin ; Severin, Daniel ; Trassl, Roland</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c435t-b4def3f424afbe93b8231b1b0d54d45eb6482b89ef432a5a4ee3e63c50fb2943</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2012</creationdate><topic>a-Si:H/μc-Si:H tandem cells</topic><topic>Applied sciences</topic><topic>Direct energy conversion and energy accumulation</topic><topic>Electrical engineering. Electrical power engineering</topic><topic>Electrical power engineering</topic><topic>Energy</topic><topic>Exact sciences and technology</topic><topic>Materials</topic><topic>Natural energy</topic><topic>PECVD</topic><topic>Photoelectric conversion</topic><topic>Photovoltaic cells</topic><topic>Photovoltaic conversion</topic><topic>Refractive index</topic><topic>Refractivity</topic><topic>Silicon</topic><topic>Silicon oxide p-layer</topic><topic>Silicon oxides</topic><topic>Silicon substrates</topic><topic>Solar cells</topic><topic>Solar cells. Photoelectrochemical cells</topic><topic>Solar energy</topic><topic>Thin film solar cells</topic><topic>Thin films</topic><topic>Zinc oxide</topic><topic>ZnO</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Schwanitz, Konrad</creatorcontrib><creatorcontrib>Klein, Stefan</creatorcontrib><creatorcontrib>Stolley, Tobias</creatorcontrib><creatorcontrib>Rohde, Martin</creatorcontrib><creatorcontrib>Severin, Daniel</creatorcontrib><creatorcontrib>Trassl, Roland</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>Electronics & Communications Abstracts</collection><collection>Environmental Engineering Abstracts</collection><collection>Mechanical & Transportation Engineering Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Environmental Sciences and Pollution Management</collection><collection>Engineering Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Solar energy materials and solar cells</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Schwanitz, Konrad</au><au>Klein, Stefan</au><au>Stolley, Tobias</au><au>Rohde, Martin</au><au>Severin, Daniel</au><au>Trassl, Roland</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Anti-reflective microcrystalline silicon oxide p-layer for thin-film silicon solar cells on ZnO</atitle><jtitle>Solar energy materials and solar cells</jtitle><date>2012-10-01</date><risdate>2012</risdate><volume>105</volume><spage>187</spage><epage>191</epage><pages>187-191</pages><issn>0927-0248</issn><eissn>1879-3398</eissn><abstract>As a result from the development of silicon thin-film solar cells that had been conducted at Applied Materials over the last few years, we present a new kind of microcrystalline silicon oxide (μc-SiOx:H) based p-layer for the application in amorphous/microcrystalline (a-Si:H/μc-Si:H) tandem solar cells on ZnO substrates. The refractive index of this p-layer can be adjusted in the range 2–3.5 and therefore serves as a refractive index matching layer between ZnO (n∼2) and silicon (n∼4). By applying such a layer the reflection of solar cells can be reduced to 3%. This results in a significant short circuit current increase in thin-film solar cells. As a follow up to the recently published results of large area thin film silicon modules by us [1,2], we describe in this paper in detail the material properties of this new silicon oxide p-layer, the optimization of electrical and optical properties in solar cells and also the impact on the light induced degradation of a-Si/μc-Si tandem junction cells.
► We reached reduction of the reflection of 2–3% with the silicon oxide p-layer. ► The absolute initial cell efficiency gain amounts 0.1% and the stable cell efficiency gain is 0.4%. ► The silicon oxide p-layer enhances the top cell current up to 0.3mA/cm². ► The relative efficiency loss by LID is 9.1–10.5%, whereas with the conventional p-layer it is 12.5%. ► stabilized module efficiencies of 10.1% on 1100× 1300mm2 glass substrates have been reached</abstract><cop>Amsterdam</cop><pub>Elsevier B.V</pub><doi>10.1016/j.solmat.2012.06.003</doi><tpages>5</tpages></addata></record> |
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subjects | a-Si:H/μc-Si:H tandem cells Applied sciences Direct energy conversion and energy accumulation Electrical engineering. Electrical power engineering Electrical power engineering Energy Exact sciences and technology Materials Natural energy PECVD Photoelectric conversion Photovoltaic cells Photovoltaic conversion Refractive index Refractivity Silicon Silicon oxide p-layer Silicon oxides Silicon substrates Solar cells Solar cells. Photoelectrochemical cells Solar energy Thin film solar cells Thin films Zinc oxide ZnO |
title | Anti-reflective microcrystalline silicon oxide p-layer for thin-film silicon solar cells on ZnO |
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