Investigation on Avalanche and Optoelectronic Response in Ga₂O₃ Photoconductive Semiconductor Switches

Photoconductive semiconductor switches (PCSSs) are noted for the rapid turn-on time and optically isolated triggering, making them suitable for high-power applications. Gallium oxide (Ga<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub>O<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3</sub>), as an ultra-wide bandgap semiconductor, is promising for use in PCSSs with ultrahigh breakdown voltage and power density. This study investigates the avalanche process of Ga<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub>O<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3</sub> PCSSs triggered by pulsed optical sources through computational simulations, focusing on the electric field distribution, carrier dynamics, and optoelectronic response. The responsivity of Ga<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub>O<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3</sub> PCSS exceeds 100 mA/W when the optical power ranges from <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$10^{4}$</tex-math> </inline-formula> to <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$10^{6}$</tex-math> </inline-formula> W/cm<sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sup>. The rise time of the switch significantly decreases from 6.5 to 2 ns with an electric field of 6 MV/cm. Results reveal that a high-density avalanche domain forms and propagates within the device with peak electric fields ranging from 6 to 8 MV/cm. Furthermore, we demonstrate that the switching time of Ga<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub>O<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3</sub> PCSS can be shorter than 500 ps. This research provides design guidance and crucial insights into the carrier dynamics of an ultrafast Ga<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub>O<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3</sub> PCSS.