2008
DOI: 10.1016/j.tsf.2008.08.136
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Epitaxially grown emitters for thin film crystalline silicon solar cells

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Cited by 20 publications
(10 citation statements)
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“…[6][7][8][9][10] Recently, PECVD epitaxial layers regained increased interest, however, as it was recognized that such layers are ideally suited to engineer silicon solar cells, either as (relatively thick) optically active absorber layers that replace the stillcostly wafer 11,12 or as thin layers for homojunction formation (electron or hole collectors, depending on the doping type). [13][14][15][16] Such thin epitaxial layers have also found application in certain high-efficiency heterojunction solar cell architectures and heterojunction field-effect transistors, illustrating that the same PECVD tools can be used to deposit various materials to engineer electronic devices. [17][18][19] Despite this, the precise influence of the plasma conditions on the electronic and microstructural quality of the grown layers has been elusive.…”
mentioning
confidence: 99%
“…[6][7][8][9][10] Recently, PECVD epitaxial layers regained increased interest, however, as it was recognized that such layers are ideally suited to engineer silicon solar cells, either as (relatively thick) optically active absorber layers that replace the stillcostly wafer 11,12 or as thin layers for homojunction formation (electron or hole collectors, depending on the doping type). [13][14][15][16] Such thin epitaxial layers have also found application in certain high-efficiency heterojunction solar cell architectures and heterojunction field-effect transistors, illustrating that the same PECVD tools can be used to deposit various materials to engineer electronic devices. [17][18][19] Despite this, the precise influence of the plasma conditions on the electronic and microstructural quality of the grown layers has been elusive.…”
mentioning
confidence: 99%
“…Doped layers (p + or n + ) are necessary in crystalline silicon (c‐Si) solar cells to form the p–n junction or to keep the minority carriers away from recombination near the contacts. These doped layers or regions in silicon can be formed by a variety of techniques such as ion‐implantation , thermal diffusion from doped silicate layers deposited in a precursor environment (POCl 3 or BBr 3 diffusion) , growth of doped epitaxial layers , use of doped silicon nanoparticles , heat treatment of solid dopant source wafers (boron nitride) , or the diffusion of dopants from doped dielectric layers . The doped dielectric layers can be deposited at low temperatures (less than 250 °C) and then subjected to drive‐in at high temperature (∼1000 °C) to diffuse the dopants inside c‐Si bulk.…”
Section: Introductionmentioning
confidence: 99%
“…Efficiencies 12.3% [5] have also been confirmed from (30μm thin) epitaxial cells built on highly doped multi-crystalline Si substrates, by Chemical Vapor Deposition (CVD), with the front and back surfaces prepared by phosphorous diffusion. Efficiencies close to 15% have been achieved from cells with an emitter grown by CVD, creating thus a front surface field, onto a base epitaxialy grown [6] via optimization of the doping and thickness of epitaxial layer. Epitaxial solar cells with porous silicon brag reflector [7] and the large-area modules, based on integrated interconnected recrystallized silicon on ceramic cells [8], represent innovative concepts, which can fulfill the requirement of lowering the cost down to 45 €ct/W p [9].…”
Section: Introductionmentioning
confidence: 99%