WSe<sub>2</sub>/β-Ga<sub>2</sub>O<sub>3</sub> p–n Heterojunction-BasedNormally Off Phototransistors forSelf-Powered UV‑C Detection

A WSe<sub>2</sub>/β-Ga<sub>2</sub>O<sub>3</sub> heterojunction (HJ)-based enhancement-mode (E-mode) phototransistor with self-powered operation was developed for ultraviolet-C (UV-C) photodetector applications, featuring a top-gate p-type WSe<sub>2</sub> (p-WSe<sub>2</sub>) and an n-type ultrawide-bandgap β-Ga<sub>2</sub>O<sub>3</sub> that serves as both the conductive channel and UV-C absorption layer. To increase the hole concentration in WSe<sub>2</sub> dry-transferred onto β-Ga<sub>2</sub>O<sub>3</sub>, the top few layers of WSe<sub>2</sub> were oxidized to tungsten oxide (WO<sub><i>x</i></sub>) (2 < <i>x</i> < 3) with a high work-function value via UV–ozone treatment. High-resolution transmission electron microscopy and energy-dispersive X-ray spectroscopy revealed excellent interface quality with atomic-scale layer uniformity in the HJ of WO<sub><i>x</i></sub>/WSe<sub>2</sub>/β-Ga<sub>2</sub>O<sub>3</sub>. The WSe<sub>2</sub>/β-Ga<sub>2</sub>O<sub>3</sub> p–n HJ diode exhibited a high rectification ratio (∼10<sup>9</sup>) and an extremely low reverse current (14 fA), allowing the demonstration of a normally off n-channel β-Ga<sub>2</sub>O<sub>3</sub> phototransistor integrated with an ultrathin p-WSe<sub>2</sub> stack. The type-II band alignment of this HJ promoted efficient separation of photogenerated electron–hole pairs under UV-C illumination, allowing us to achieve excellent optoelectronic performance under standalone operation. Without an external power source, the WSe<sub>2</sub>/β-Ga<sub>2</sub>O<sub>3</sub> E-mode phototransistor exhibited excellent optoelectronic performance, including responsivity of 2.1 A W<sup>–1</sup>, a photo-to-dark current ratio of 1.5 × 10<sup>3</sup>, external quantum efficiency of 10.2%, specific detectivity of 6.4 × 10<sup>7</sup> Jones, UV-A selectivity with a rejection ratio (<i>R</i><sub>254nm</sub>/<i>R</i><sub>365nm</sub>) of 4, and a fast response without persistent photoconductivity. These findings highlight the potential of p-WSe<sub>2</sub>/β-Ga<sub>2</sub>O<sub>3</sub> heterostructure UV-C phototransistors with high sensitivity and energy efficiency because of their compact and standalone deep-UV optoelectronic architecture.

Publication Details

Journal
Figshare
Published
2025-03-24
DOI
https://doi.org/10.1021/acsphotonics.4c02595.s001
Primary Topic
Plant pathogens and resistance mechanisms
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article
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article

WSe2/β-Ga2O3 p–n Heterojunction-BasedNormally Off Phototransistors forSelf-Powered UV‑C Detection

Figshare
Plant pathogens and resistance mechanisms
article

WSe2/β-Ga2O3 p–n Heterojunction-BasedNormally Off Phototransistors forSelf-Powered UV‑C Detection

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Abstract

A WSe<sub>2</sub>/β-Ga<sub>2</sub>O<sub>3</sub> heterojunction (HJ)-based enhancement-mode (E-mode) phototransistor with self-powered operation was developed for ultraviolet-C (UV-C) photodetector applications, featuring a top-gate p-type WSe<sub>2</sub> (p-WSe<sub>2</sub>) and an n-type ultrawide-bandgap β-Ga<sub>2</sub>O<sub>3</sub> that serves as both the conductive channel and UV-C absorption layer. To increase the hole concentration in WSe<sub>2</sub> dry-transferred onto β-Ga<sub>2</sub>O<sub>3</sub>, the top few layers of WSe<sub>2</sub> were oxidized to tungsten oxide (WO<sub><i>x</i></sub>) (2 < <i>x</i> < 3) with a high work-function value via UV–ozone treatment. High-resolution transmission electron microscopy and energy-dispersive X-ray spectroscopy revealed excellent interface quality with atomic-scale layer uniformity in the HJ of WO<sub><i>x</i></sub>/WSe<sub>2</sub>/β-Ga<sub>2</sub>O<sub>3</sub>. The WSe<sub>2</sub>/β-Ga<sub>2</sub>O<sub>3</sub> p–n HJ diode exhibited a high rectification ratio (∼10<sup>9</sup>) and an extremely low reverse current (14 fA), allowing the demonstration of a normally off n-channel β-Ga<sub>2</sub>O<sub>3</sub> phototransistor integrated with an ultrathin p-WSe<sub>2</sub> stack. The type-II band alignment of this HJ promoted efficient separation of photogenerated electron–hole pairs under UV-C illumination, allowing us to achieve excellent optoelectronic performance under standalone operation. Without an external power source, the WSe<sub>2</sub>/β-Ga<sub>2</sub>O<sub>3</sub> E-mode phototransistor exhibited excellent optoelectronic performance, including responsivity of 2.1 A W<sup>–1</sup>, a photo-to-dark current ratio of 1.5 × 10<sup>3</sup>, external quantum efficiency of 10.2%, specific detectivity of 6.4 × 10<sup>7</sup> Jones, UV-A selectivity with a rejection ratio (<i>R</i><sub>254nm</sub>/<i>R</i><sub>365nm</sub>) of 4, and a fast response without persistent photoconductivity. These findings highlight the potential of p-WSe<sub>2</sub>/β-Ga<sub>2</sub>O<sub>3</sub> heterostructure UV-C phototransistors with high sensitivity and energy efficiency because of their compact and standalone deep-UV optoelectronic architecture.

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