Abstract

The formation of heavily doped p <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">+</sup> region on p-type silicon substrates using laser doping through a layer of ALD AlO <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">x</sub> is studied. A 532 nm continuous wave (CW) laser is used to incorporate Al atoms from the AlO <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">x</sub> layers to form p <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">+</sup> silicon. The p <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">+</sup> regions formed through laser doping are found to be affected by various parameters such as laser speed and power. Sheet resistances as low as 10 Ω/□ were achieved using a power of 15 W and laser scanning speed of 0.5 m/s. The impact of the laser doping process on effective minority carrier lifetime is investigated using only the AlO <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">x</sub> layer as a dopant source, as well as with the addition of a Boron dopant source. Laser doping boron have better protection by introducing a lifetime drop from 67 μs to 57.7 μs after laser doping comparing to the lifetime drop of laser doping AlO <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">x</sub> from 62.5 μs to 46.1 μs. However, the addition of a boron spin on dopant source may induce voids in the laser doped region.

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