Efficiency enhancement of a-Si:H single junction solar cells by a-Ge:H incorporation at the p + a-SiC:H/transparent conducting oxide interface
Carbon (C) incorporation in the p + hydrogenated amorphous silicon (a-SiC:H) is highly desirable for a-Si:H based solar cells because of the following reasons: (i) it increases the band gap of the p + layer to ∼2 eV, which allows a majority of the sun light to pass through the thin p + layer (∼15 nm...
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container_title | Applied physics letters |
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creator | Kim, Jeehwan Abou-Kandil, Ahmed I. Hong, Augustin J. Saad, Mohamed M. Sadana, Devendra K. Chen, Tze-Chiang |
description | Carbon (C) incorporation in the p
+
hydrogenated amorphous silicon (a-SiC:H) is highly desirable for a-Si:H based solar cells because of the following reasons: (i) it increases the band gap of the p
+
layer to ∼2 eV, which allows a majority of the sun light to pass through the thin p
+
layer (∼15 nm) and get absorbed in the underlying intrinsic a-Si:H layer, and (ii) it enhances built-in potential of the a-Si:H p-i-n stack, resulting in enhanced short circuit current (J
SC
) and open circuit voltage (V
OC
). Hence, it is a desire to incorporate the highest possible C % in the p
+
a-Si:H. However, C incorporation results in a Schottky barrier at the p
+
a-SiC:H/transparent conducting oxide (TCO) interface, which degrades the fill factor (FF) of the solar cell. In this paper, we present a method that increases the C incorporation in p
+
a-SiC:H but without adversely affecting the FF, by adding a thin layer of hydrogenated amorphous germanium (a-Ge:H) buffer at the p
+
a-SiC:H/TCO interface. The presence of a-Ge:H can either minimize or eliminate the Schottky barrier. We demonstrate ∼25% enhanced efficiency of the a-Si:H solar cell by using the a-Ge:H interfacial buffer compared to that without an a-Ge:H interfacial layer. |
doi_str_mv | 10.1063/1.3619185 |
format | Article |
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+
hydrogenated amorphous silicon (a-SiC:H) is highly desirable for a-Si:H based solar cells because of the following reasons: (i) it increases the band gap of the p
+
layer to ∼2 eV, which allows a majority of the sun light to pass through the thin p
+
layer (∼15 nm) and get absorbed in the underlying intrinsic a-Si:H layer, and (ii) it enhances built-in potential of the a-Si:H p-i-n stack, resulting in enhanced short circuit current (J
SC
) and open circuit voltage (V
OC
). Hence, it is a desire to incorporate the highest possible C % in the p
+
a-Si:H. However, C incorporation results in a Schottky barrier at the p
+
a-SiC:H/transparent conducting oxide (TCO) interface, which degrades the fill factor (FF) of the solar cell. In this paper, we present a method that increases the C incorporation in p
+
a-SiC:H but without adversely affecting the FF, by adding a thin layer of hydrogenated amorphous germanium (a-Ge:H) buffer at the p
+
a-SiC:H/TCO interface. The presence of a-Ge:H can either minimize or eliminate the Schottky barrier. We demonstrate ∼25% enhanced efficiency of the a-Si:H solar cell by using the a-Ge:H interfacial buffer compared to that without an a-Ge:H interfacial layer.</description><identifier>ISSN: 0003-6951</identifier><identifier>EISSN: 1077-3118</identifier><identifier>DOI: 10.1063/1.3619185</identifier><identifier>CODEN: APPLAB</identifier><language>eng</language><publisher>American Institute of Physics</publisher><ispartof>Applied physics letters, 2011-08, Vol.99 (6), p.062102-062102-3</ispartof><rights>2011 American Institute of Physics</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c284t-9c8b1f1fd0c328c664298ae5a2fa3642fb895841f569d6979cc27a2483bd08103</citedby><cites>FETCH-LOGICAL-c284t-9c8b1f1fd0c328c664298ae5a2fa3642fb895841f569d6979cc27a2483bd08103</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://pubs.aip.org/apl/article-lookup/doi/10.1063/1.3619185$$EHTML$$P50$$Gscitation$$H</linktohtml><link.rule.ids>314,780,784,794,1559,4512,27924,27925,76384,76390</link.rule.ids></links><search><creatorcontrib>Kim, Jeehwan</creatorcontrib><creatorcontrib>Abou-Kandil, Ahmed I.</creatorcontrib><creatorcontrib>Hong, Augustin J.</creatorcontrib><creatorcontrib>Saad, Mohamed M.</creatorcontrib><creatorcontrib>Sadana, Devendra K.</creatorcontrib><creatorcontrib>Chen, Tze-Chiang</creatorcontrib><title>Efficiency enhancement of a-Si:H single junction solar cells by a-Ge:H incorporation at the p + a-SiC:H/transparent conducting oxide interface</title><title>Applied physics letters</title><description>Carbon (C) incorporation in the p
+
hydrogenated amorphous silicon (a-SiC:H) is highly desirable for a-Si:H based solar cells because of the following reasons: (i) it increases the band gap of the p
+
layer to ∼2 eV, which allows a majority of the sun light to pass through the thin p
+
layer (∼15 nm) and get absorbed in the underlying intrinsic a-Si:H layer, and (ii) it enhances built-in potential of the a-Si:H p-i-n stack, resulting in enhanced short circuit current (J
SC
) and open circuit voltage (V
OC
). Hence, it is a desire to incorporate the highest possible C % in the p
+
a-Si:H. However, C incorporation results in a Schottky barrier at the p
+
a-SiC:H/transparent conducting oxide (TCO) interface, which degrades the fill factor (FF) of the solar cell. In this paper, we present a method that increases the C incorporation in p
+
a-SiC:H but without adversely affecting the FF, by adding a thin layer of hydrogenated amorphous germanium (a-Ge:H) buffer at the p
+
a-SiC:H/TCO interface. The presence of a-Ge:H can either minimize or eliminate the Schottky barrier. We demonstrate ∼25% enhanced efficiency of the a-Si:H solar cell by using the a-Ge:H interfacial buffer compared to that without an a-Ge:H interfacial layer.</description><issn>0003-6951</issn><issn>1077-3118</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2011</creationdate><recordtype>article</recordtype><recordid>eNp1kMtKAzEUQIMoWKsL_yBbkWmTyTySLgQptRUKLtT1kLmTtCnTZEhSsD_hNzt9oCtXlwvnHrgHoXtKRpQUbExHrKCC8vwCDSgpy4RRyi_RgBDCkkLk9BrdhLDp1zxlbIC-Z1obMMrCHiu7lhbUVtmIncYyeTeTBQ7GrlqFNzsL0TiLg2ulx6DaNuB631Nz1VPGgvOd8_LIyIjjWuEOPx4t08liHL20oZP-IAdnm11vsyvsvkyj-uuovJagbtGVlm1Qd-c5RJ8vs4_pIlm-zV-nz8sEUp7FRACvqaa6IcBSDkWRpYJLlctUS9YvuuYi5xnVeSGaQpQCIC1lmnFWN4RTwobo4eQF70LwSledN1vp9xUl1SFkRatzyJ59OrEBTDz-9z_8V7P6rcl-ALvOe2Y</recordid><startdate>20110808</startdate><enddate>20110808</enddate><creator>Kim, Jeehwan</creator><creator>Abou-Kandil, Ahmed I.</creator><creator>Hong, Augustin J.</creator><creator>Saad, Mohamed M.</creator><creator>Sadana, Devendra K.</creator><creator>Chen, Tze-Chiang</creator><general>American Institute of Physics</general><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>20110808</creationdate><title>Efficiency enhancement of a-Si:H single junction solar cells by a-Ge:H incorporation at the p + a-SiC:H/transparent conducting oxide interface</title><author>Kim, Jeehwan ; Abou-Kandil, Ahmed I. ; Hong, Augustin J. ; Saad, Mohamed M. ; Sadana, Devendra K. ; Chen, Tze-Chiang</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c284t-9c8b1f1fd0c328c664298ae5a2fa3642fb895841f569d6979cc27a2483bd08103</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2011</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Kim, Jeehwan</creatorcontrib><creatorcontrib>Abou-Kandil, Ahmed I.</creatorcontrib><creatorcontrib>Hong, Augustin J.</creatorcontrib><creatorcontrib>Saad, Mohamed M.</creatorcontrib><creatorcontrib>Sadana, Devendra K.</creatorcontrib><creatorcontrib>Chen, Tze-Chiang</creatorcontrib><collection>CrossRef</collection><jtitle>Applied physics letters</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Kim, Jeehwan</au><au>Abou-Kandil, Ahmed I.</au><au>Hong, Augustin J.</au><au>Saad, Mohamed M.</au><au>Sadana, Devendra K.</au><au>Chen, Tze-Chiang</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Efficiency enhancement of a-Si:H single junction solar cells by a-Ge:H incorporation at the p + a-SiC:H/transparent conducting oxide interface</atitle><jtitle>Applied physics letters</jtitle><date>2011-08-08</date><risdate>2011</risdate><volume>99</volume><issue>6</issue><spage>062102</spage><epage>062102-3</epage><pages>062102-062102-3</pages><issn>0003-6951</issn><eissn>1077-3118</eissn><coden>APPLAB</coden><abstract>Carbon (C) incorporation in the p
+
hydrogenated amorphous silicon (a-SiC:H) is highly desirable for a-Si:H based solar cells because of the following reasons: (i) it increases the band gap of the p
+
layer to ∼2 eV, which allows a majority of the sun light to pass through the thin p
+
layer (∼15 nm) and get absorbed in the underlying intrinsic a-Si:H layer, and (ii) it enhances built-in potential of the a-Si:H p-i-n stack, resulting in enhanced short circuit current (J
SC
) and open circuit voltage (V
OC
). Hence, it is a desire to incorporate the highest possible C % in the p
+
a-Si:H. However, C incorporation results in a Schottky barrier at the p
+
a-SiC:H/transparent conducting oxide (TCO) interface, which degrades the fill factor (FF) of the solar cell. In this paper, we present a method that increases the C incorporation in p
+
a-SiC:H but without adversely affecting the FF, by adding a thin layer of hydrogenated amorphous germanium (a-Ge:H) buffer at the p
+
a-SiC:H/TCO interface. The presence of a-Ge:H can either minimize or eliminate the Schottky barrier. We demonstrate ∼25% enhanced efficiency of the a-Si:H solar cell by using the a-Ge:H interfacial buffer compared to that without an a-Ge:H interfacial layer.</abstract><pub>American Institute of Physics</pub><doi>10.1063/1.3619185</doi></addata></record> |
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source | AIP Journals Complete; AIP Digital Archive; Alma/SFX Local Collection |
title | Efficiency enhancement of a-Si:H single junction solar cells by a-Ge:H incorporation at the p + a-SiC:H/transparent conducting oxide interface |
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