Effect of Crystallographic Orientation and Nanoscale Surface Morphology on Poly-Si/SiOx Contacts for Silicon Solar Cells
Author(s) -
Abhijit S. Kale,
William Nemeth,
Harvey Guthrey,
Sanjini U. Nanayakkara,
Vincenzo LaSalvia,
San Theingi,
Dawn Findley,
Matthew Page,
Mowafak AlJassim,
David L. Young,
Paul Stradins,
Sumit Agarwal
Publication year - 2019
Publication title -
acs applied materials and interfaces
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 2.535
H-Index - 228
eISSN - 1944-8252
pISSN - 1944-8244
DOI - 10.1021/acsami.9b11889
Subject(s) - materials science , nanoscopic scale , silicon , morphology (biology) , orientation (vector space) , crystallography , nanotechnology , surface (topology) , engineering physics , optoelectronics , geometry , chemistry , genetics , mathematics , engineering , biology
High-efficiency crystalline silicon (Si) solar cells require textured surfaces for efficient light trapping. However, passivation of a textured surface to reduce carrier recombination is difficult. Here, we relate the electrical properties of cells fabricated on a KOH-etched, random pyramidal-textured Si surface to the nanostructure of the passivated contact and the textured surface morphology. The effects of both microscopic pyramidal morphology and nanoscale surface roughness on passivated contacts consisting of polycrystalline Si ( poly -Si) deposited on top of an ultrathin, 1.5-2.2 nm, SiO x layer are investigated. Using atomic force microscopy, we show a pyramid face, which is predominantly a Si(111) plane to be significantly rougher than a polished Si(111) surface. This roughness results in a nonuniform SiO x layer as determined by transmission electron microscopy of a poly -Si/SiO x contact. Our device measurements also show an overall more resistive and hence a thicker SiO x layer over the pyramidal surface as compared to a polished Si(111) surface, which we relate to increased surface roughness. Using electron-beam-induced current measurements of poly -Si/SiO x contacts, we further show that the SiO x layer near the pyramid valleys is preferentially more conducting and hence likely thinner than over pyramid tips, edges, and faces. Hence, both the microscopic pyramidal morphology and nanoscale roughness lead to a nonuniform SiO x layer, thus leading to poor poly -Si/SiO x contact passivation. Finally, we report >21% efficient and ≥80% fill-factor front/back poly -Si/SiO x solar cells on both single-side and double-side textured wafers without the use of transparent conductive oxide layers, and show that the poorer contact passivation on a textured surface is limited to boron-doped poly -Si/SiO x contacts.
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