کد مقاله | کد نشریه | سال انتشار | مقاله انگلیسی | نسخه تمام متن |
---|---|---|---|---|
77790 | 49305 | 2015 | 10 صفحه PDF | دانلود رایگان |
![عکس صفحه اول مقاله: Impact of boron doping profiles on the specific contact resistance of screen printed Ag–Al contacts on silicon Impact of boron doping profiles on the specific contact resistance of screen printed Ag–Al contacts on silicon](/preview/png/77790.png)
• Specific contact resistance ρC between Ag–Al contact and boron-doped silicon.
• Boron doping profiles with deeper junction feature lower ρC.
• Crystallite penetration depths between several 100 nm and a few microns.
• Analytical model basing on crystallites can describe the measured ρC.
• Doping depletion zone negligible with respect to ρC for sufficiently deep crystallites.
For the contacting of boron-doped emitters with screen-printed metallization in n-type silicon solar cells, usually a small amount of aluminum is added to the silver pastes. To date, low specific contact resistances ρC in the range of a few mΩ cm2 have only been achieved with these so-called silver–aluminum (Ag–Al) pastes. Within this work, ρC is experimentally determined for two Ag–Al pastes for three different boron-doped emitters on alkaline textured and passivated silicon surfaces. The investigated boron doping profiles feature almost identical rising curve progressions up to a depth of ≈60 nm (which corresponds to the depletion zone), with a maximum dopant concentration Nmax≈8·1019 cm−3. However, they have different junction depths between 570 nm and 980 nm. This work shows that the dopant concentrations with values well below Nmax following the depletion zone significantly affect the measured ρC: the deeper the junction, the lower ρC. This behavior is observed for both investigated Ag–Al pastes. For example, the mean ρC for paste Ag–Al1 decreases from ρC≈4 mΩ cm2, determined on a 570 nm deep doping profile, to ρC≈2 mΩ cm2, determined on a 980 nm deep one. By using an analytical model to calculate ρC with dependence on e.g. dopant concentration, metal crystallite coverage fraction, and crystallite penetration depth, the lower ρC for deeper profiles can be explained by crystallites with penetration depths of several 100 nm. The calculations also reveal that the impact of the depletion zone is negligible with respect to ρC for crystallites deeper than ≈100 nm.
Journal: Solar Energy Materials and Solar Cells - Volume 142, November 2015, Pages 2–11