Passivation mechanism in silicon heterojunction solar cells with intrinsic hydrogenated amorphous silicon oxide layers
In this work, we use intrinsic hydrogenated amorphous silicon oxide layers (a-SiO x :H) with varying oxygen content (c O) but similar hydrogen content to passivate the crystalline silicon wafers. Using our deposition conditions, we obtain an effective lifetime (τ eff) above 5 ms for c O ≤ 6 at. % fo...
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container_title | Journal of applied physics |
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creator | Deligiannis, Dimitrios van Vliet, Jeroen Vasudevan, Ravi van Swaaij, René A. C. M. M. Zeman, Miro |
description | In this work, we use intrinsic hydrogenated amorphous silicon oxide layers (a-SiO
x
:H) with varying oxygen content (c
O) but similar hydrogen content to passivate the crystalline silicon wafers. Using our deposition conditions, we obtain an effective lifetime (τ
eff) above 5 ms for c
O ≤ 6 at. % for passivation layers with a thickness of 36 ± 2 nm. We subsequently reduce the thickness of the layers using an accurate wet etching method to ∼7 nm and deposit p- and n-type doped layers fabricating a device structure. After the deposition of the doped layers, τ
eff appears to be predominantly determined by the doped layers themselves and is less dependent on the c
O of the a-SiO
x
:H layers. The results suggest that τ
eff is determined by the field-effect rather than by chemical passivation. |
doi_str_mv | 10.1063/1.4977242 |
format | Article |
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x
:H) with varying oxygen content (c
O) but similar hydrogen content to passivate the crystalline silicon wafers. Using our deposition conditions, we obtain an effective lifetime (τ
eff) above 5 ms for c
O ≤ 6 at. % for passivation layers with a thickness of 36 ± 2 nm. We subsequently reduce the thickness of the layers using an accurate wet etching method to ∼7 nm and deposit p- and n-type doped layers fabricating a device structure. After the deposition of the doped layers, τ
eff appears to be predominantly determined by the doped layers themselves and is less dependent on the c
O of the a-SiO
x
:H layers. The results suggest that τ
eff is determined by the field-effect rather than by chemical passivation.</description><identifier>ISSN: 0021-8979</identifier><identifier>EISSN: 1089-7550</identifier><identifier>DOI: 10.1063/1.4977242</identifier><identifier>CODEN: JAPIAU</identifier><language>eng</language><publisher>Melville: American Institute of Physics</publisher><subject>Amorphous silicon ; Applied physics ; Deposition ; Heterojunctions ; Hydrogen storage ; Hydrogenation ; Organic chemistry ; Oxygen content ; Passivity ; Photovoltaic cells ; Silicon oxides ; Silicon wafers ; Solar cells ; Thickness</subject><ispartof>Journal of applied physics, 2017-02, Vol.121 (8)</ispartof><rights>Author(s)</rights><rights>2017 Author(s). Published by AIP Publishing.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c327t-9a6b38e3a164ca4a7fce8fa2534283beb1a187db7d1e093e42015153239615e03</citedby><cites>FETCH-LOGICAL-c327t-9a6b38e3a164ca4a7fce8fa2534283beb1a187db7d1e093e42015153239615e03</cites><orcidid>0000-0002-0275-0791</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://pubs.aip.org/jap/article-lookup/doi/10.1063/1.4977242$$EHTML$$P50$$Gscitation$$H</linktohtml><link.rule.ids>314,780,784,794,4512,27924,27925,76384</link.rule.ids></links><search><creatorcontrib>Deligiannis, Dimitrios</creatorcontrib><creatorcontrib>van Vliet, Jeroen</creatorcontrib><creatorcontrib>Vasudevan, Ravi</creatorcontrib><creatorcontrib>van Swaaij, René A. C. M. M.</creatorcontrib><creatorcontrib>Zeman, Miro</creatorcontrib><title>Passivation mechanism in silicon heterojunction solar cells with intrinsic hydrogenated amorphous silicon oxide layers</title><title>Journal of applied physics</title><description>In this work, we use intrinsic hydrogenated amorphous silicon oxide layers (a-SiO
x
:H) with varying oxygen content (c
O) but similar hydrogen content to passivate the crystalline silicon wafers. Using our deposition conditions, we obtain an effective lifetime (τ
eff) above 5 ms for c
O ≤ 6 at. % for passivation layers with a thickness of 36 ± 2 nm. We subsequently reduce the thickness of the layers using an accurate wet etching method to ∼7 nm and deposit p- and n-type doped layers fabricating a device structure. After the deposition of the doped layers, τ
eff appears to be predominantly determined by the doped layers themselves and is less dependent on the c
O of the a-SiO
x
:H layers. The results suggest that τ
eff is determined by the field-effect rather than by chemical passivation.</description><subject>Amorphous silicon</subject><subject>Applied physics</subject><subject>Deposition</subject><subject>Heterojunctions</subject><subject>Hydrogen storage</subject><subject>Hydrogenation</subject><subject>Organic chemistry</subject><subject>Oxygen content</subject><subject>Passivity</subject><subject>Photovoltaic cells</subject><subject>Silicon oxides</subject><subject>Silicon wafers</subject><subject>Solar cells</subject><subject>Thickness</subject><issn>0021-8979</issn><issn>1089-7550</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2017</creationdate><recordtype>article</recordtype><recordid>eNp90F9LwzAUBfAgCs7pg9-g4JNCZ27SNs2jiP9goA_6HNL01ma0zUza6b69dRvzQfDpwuXHOXAIOQc6A5rxa5glUgiWsAMyAZrLWKQpPSQTShnEuRTymJyEsKAUIOdyQlYvOgS70r11XdSiqXVnQxvZLgq2sWZ81tijd4uhMxsTXKN9ZLBpQvRp-3qkvbddsCaq16V379jpHstIt84vazeEfZD7siVGjV6jD6fkqNJNwLPdnZK3-7vX28d4_vzwdHszjw1noo-lzgqeI9eQJUYnWlQG80qzlCcs5wUWoCEXZSFKQCo5JoxCCilnXGaQIuVTcrHNXXr3MWDo1cINvhsrFQOWpGmS8WxUl1tlvAvBY6WW3rbarxVQ9TOrArWbdbRXWxuM7Tez7fHK-V-olmX1H_6b_A0s4oib</recordid><startdate>20170228</startdate><enddate>20170228</enddate><creator>Deligiannis, Dimitrios</creator><creator>van Vliet, Jeroen</creator><creator>Vasudevan, Ravi</creator><creator>van Swaaij, René A. C. M. M.</creator><creator>Zeman, Miro</creator><general>American Institute of Physics</general><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><orcidid>https://orcid.org/0000-0002-0275-0791</orcidid></search><sort><creationdate>20170228</creationdate><title>Passivation mechanism in silicon heterojunction solar cells with intrinsic hydrogenated amorphous silicon oxide layers</title><author>Deligiannis, Dimitrios ; van Vliet, Jeroen ; Vasudevan, Ravi ; van Swaaij, René A. C. M. M. ; Zeman, Miro</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c327t-9a6b38e3a164ca4a7fce8fa2534283beb1a187db7d1e093e42015153239615e03</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2017</creationdate><topic>Amorphous silicon</topic><topic>Applied physics</topic><topic>Deposition</topic><topic>Heterojunctions</topic><topic>Hydrogen storage</topic><topic>Hydrogenation</topic><topic>Organic chemistry</topic><topic>Oxygen content</topic><topic>Passivity</topic><topic>Photovoltaic cells</topic><topic>Silicon oxides</topic><topic>Silicon wafers</topic><topic>Solar cells</topic><topic>Thickness</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Deligiannis, Dimitrios</creatorcontrib><creatorcontrib>van Vliet, Jeroen</creatorcontrib><creatorcontrib>Vasudevan, Ravi</creatorcontrib><creatorcontrib>van Swaaij, René A. C. M. M.</creatorcontrib><creatorcontrib>Zeman, Miro</creatorcontrib><collection>CrossRef</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Journal of applied physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Deligiannis, Dimitrios</au><au>van Vliet, Jeroen</au><au>Vasudevan, Ravi</au><au>van Swaaij, René A. C. M. M.</au><au>Zeman, Miro</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Passivation mechanism in silicon heterojunction solar cells with intrinsic hydrogenated amorphous silicon oxide layers</atitle><jtitle>Journal of applied physics</jtitle><date>2017-02-28</date><risdate>2017</risdate><volume>121</volume><issue>8</issue><issn>0021-8979</issn><eissn>1089-7550</eissn><coden>JAPIAU</coden><abstract>In this work, we use intrinsic hydrogenated amorphous silicon oxide layers (a-SiO
x
:H) with varying oxygen content (c
O) but similar hydrogen content to passivate the crystalline silicon wafers. Using our deposition conditions, we obtain an effective lifetime (τ
eff) above 5 ms for c
O ≤ 6 at. % for passivation layers with a thickness of 36 ± 2 nm. We subsequently reduce the thickness of the layers using an accurate wet etching method to ∼7 nm and deposit p- and n-type doped layers fabricating a device structure. After the deposition of the doped layers, τ
eff appears to be predominantly determined by the doped layers themselves and is less dependent on the c
O of the a-SiO
x
:H layers. The results suggest that τ
eff is determined by the field-effect rather than by chemical passivation.</abstract><cop>Melville</cop><pub>American Institute of Physics</pub><doi>10.1063/1.4977242</doi><tpages>7</tpages><orcidid>https://orcid.org/0000-0002-0275-0791</orcidid></addata></record> |
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source | AIP Journals Complete; Alma/SFX Local Collection |
subjects | Amorphous silicon Applied physics Deposition Heterojunctions Hydrogen storage Hydrogenation Organic chemistry Oxygen content Passivity Photovoltaic cells Silicon oxides Silicon wafers Solar cells Thickness |
title | Passivation mechanism in silicon heterojunction solar cells with intrinsic hydrogenated amorphous silicon oxide layers |
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