Hydrogen-doped indium oxide/indium tin oxide bilayers for high-efficiency silicon heterojunction solar cells
Identifieur interne : 000B73 ( Main/Repository ); précédent : 000B72; suivant : 000B74Hydrogen-doped indium oxide/indium tin oxide bilayers for high-efficiency silicon heterojunction solar cells
Auteurs : RBID : Pascal:13-0210440Descripteurs français
- Pascal (Inist)
- Matériau dopé, Couche ITO, Addition étain, Rendement élevé, Cellule solaire silicium, Hétérojonction, Perte optique, Echange commercial, Porteur libre, Résistivité couche, Mobilité électron, Etude comparative, Résistance contact, Interface entrée sortie, Evaluation performance, Cellule solaire, Sérigraphie, Hydrogène, Oxyde d'indium, Bicouche, Matériau conducteur, Matériau transparent, Argent, Silicium, Marché électricité, Economie réseau électrique, ITO.
- Wicri :
English descriptors
- KwdEn :
- Bilayers, Comparative study, Conducting material, Contact resistance, Doped materials, Electron mobility, Free carrier, Heterojunction, High efficiency, Hydrogen, ITO layers, Indium oxide, Input output interface, Optical losses, Performance evaluation, Power markets, Power system economics, Serigraphy, Sheet resistivity, Silicon, Silicon solar cells, Silver, Solar cell, Tin addition, Trade, Transparent material.
Abstract
The front transparent conductive oxide layer is a source of significant optical and electrical losses in silicon heterojunction solar cells because of the trade-off between free-carrier absorption and sheet resistance. We demonstrate that hydrogen-doped indium oxide (IO:H), which has an electron mobility of over 100 cm2/V s, reduces these losses compared to traditional, low-mobility transparent conductive oxides, but suffers from high contact resistance at the interface of the IO:H layer and the silver front electrode grid. This problem is avoided by inserting a thin indium tin oxide (ITO) layer at the IO:H/silver interface. Such IO:H/ITO bilayers have low contact resistance, sheet resistance, and free-carrier absorption, and outperform IO:H-only or ITO-only layers in solar cells. We report a certified efficiency of 22.1% for a 4-cm2 screen-printed silicon heterojunction solar cell employing an IO:H/ITO bilayer as the front transparent conductive oxide.
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Pascal:13-0210440Le document en format XML
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<term>Serigraphy</term>
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<term>Etude comparative</term>
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<term>Interface entrée sortie</term>
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<front><div type="abstract" xml:lang="en">The front transparent conductive oxide layer is a source of significant optical and electrical losses in silicon heterojunction solar cells because of the trade-off between free-carrier absorption and sheet resistance. We demonstrate that hydrogen-doped indium oxide (IO:H), which has an electron mobility of over 100 cm<sup>2</sup>
/V s, reduces these losses compared to traditional, low-mobility transparent conductive oxides, but suffers from high contact resistance at the interface of the IO:H layer and the silver front electrode grid. This problem is avoided by inserting a thin indium tin oxide (ITO) layer at the IO:H/silver interface. Such IO:H/ITO bilayers have low contact resistance, sheet resistance, and free-carrier absorption, and outperform IO:H-only or ITO-only layers in solar cells. We report a certified efficiency of 22.1% for a 4-cm<sup>2</sup>
screen-printed silicon heterojunction solar cell employing an IO:H/ITO bilayer as the front transparent conductive oxide.</div>
</front>
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<fC01 i1="01" l="ENG"><s0>The front transparent conductive oxide layer is a source of significant optical and electrical losses in silicon heterojunction solar cells because of the trade-off between free-carrier absorption and sheet resistance. We demonstrate that hydrogen-doped indium oxide (IO:H), which has an electron mobility of over 100 cm<sup>2</sup>
/V s, reduces these losses compared to traditional, low-mobility transparent conductive oxides, but suffers from high contact resistance at the interface of the IO:H layer and the silver front electrode grid. This problem is avoided by inserting a thin indium tin oxide (ITO) layer at the IO:H/silver interface. Such IO:H/ITO bilayers have low contact resistance, sheet resistance, and free-carrier absorption, and outperform IO:H-only or ITO-only layers in solar cells. We report a certified efficiency of 22.1% for a 4-cm<sup>2</sup>
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</fC03>
<fC03 i1="19" i2="X" l="SPA"><s0>Indio óxido</s0>
<s5>23</s5>
</fC03>
<fC03 i1="20" i2="3" l="FRE"><s0>Bicouche</s0>
<s5>24</s5>
</fC03>
<fC03 i1="20" i2="3" l="ENG"><s0>Bilayers</s0>
<s5>24</s5>
</fC03>
<fC03 i1="21" i2="X" l="FRE"><s0>Matériau conducteur</s0>
<s5>25</s5>
</fC03>
<fC03 i1="21" i2="X" l="ENG"><s0>Conducting material</s0>
<s5>25</s5>
</fC03>
<fC03 i1="21" i2="X" l="SPA"><s0>Material conductor</s0>
<s5>25</s5>
</fC03>
<fC03 i1="22" i2="X" l="FRE"><s0>Matériau transparent</s0>
<s5>26</s5>
</fC03>
<fC03 i1="22" i2="X" l="ENG"><s0>Transparent material</s0>
<s5>26</s5>
</fC03>
<fC03 i1="22" i2="X" l="SPA"><s0>Material transparente</s0>
<s5>26</s5>
</fC03>
<fC03 i1="23" i2="X" l="FRE"><s0>Argent</s0>
<s2>NC</s2>
<s2>FX</s2>
<s5>27</s5>
</fC03>
<fC03 i1="23" i2="X" l="ENG"><s0>Silver</s0>
<s2>NC</s2>
<s2>FX</s2>
<s5>27</s5>
</fC03>
<fC03 i1="23" i2="X" l="SPA"><s0>Plata</s0>
<s2>NC</s2>
<s2>FX</s2>
<s5>27</s5>
</fC03>
<fC03 i1="24" i2="X" l="FRE"><s0>Silicium</s0>
<s2>NC</s2>
<s5>28</s5>
</fC03>
<fC03 i1="24" i2="X" l="ENG"><s0>Silicon</s0>
<s2>NC</s2>
<s5>28</s5>
</fC03>
<fC03 i1="24" i2="X" l="SPA"><s0>Silicio</s0>
<s2>NC</s2>
<s5>28</s5>
</fC03>
<fC03 i1="25" i2="3" l="FRE"><s0>Marché électricité</s0>
<s5>46</s5>
</fC03>
<fC03 i1="25" i2="3" l="ENG"><s0>Power markets</s0>
<s5>46</s5>
</fC03>
<fC03 i1="26" i2="3" l="FRE"><s0>Economie réseau électrique</s0>
<s5>47</s5>
</fC03>
<fC03 i1="26" i2="3" l="ENG"><s0>Power system economics</s0>
<s5>47</s5>
</fC03>
<fC03 i1="27" i2="X" l="FRE"><s0>ITO</s0>
<s4>INC</s4>
<s5>82</s5>
</fC03>
<fN21><s1>196</s1>
</fN21>
<fN44 i1="01"><s1>OTO</s1>
</fN44>
<fN82><s1>OTO</s1>
</fN82>
</pA>
</standard>
</inist>
</record>
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