Abstract

In this work, β-Ga<sub>2</sub>O<sub>3</sub> films with different thickness are prepared on (001) sapphire substrates at room temperature by the radio frequency magnetron sputtering technology, then the samples are annealed in an Ar atmosphere at 800 ℃ for 1h. The effects of film thickness on the phase composition, surface morphology, optical property, and photoelectric detection performance are investigated using XRD, SEM, UV-Vis spectrophotometer, PL photoluminescence spectrometer, and Keithley 4200-SCS semiconductor characterization system. The results show that as the film thickness increases, the film crystallinity is improved, films with a thickness of 840 nm exhibit best quality, while those with a thickness of 1050 nm declines a little in quality. The β-Ga<sub>2</sub>O<sub>3</sub> films with different thickness exhibit obvious ultraviolet light absorption in the solar-blind region with wavelengths of 200–300 nm, and the bandgap width increases with the film thickness increasing. All the β-Ga<sub>2</sub>O<sub>3</sub> films show a broad UV-green light emission peaks in a wavelength range of 350–600 nm. As the film thickness increases, the intensities of the emission peaks of ultraviolet, violet, and blue light are greatly reduced, indicating that oxygen vacancy-related defects (<i>V</i><sub>O</sub>, <i>V</i><sub>Ga</sub>–<i>V</i><sub>O</sub>) are greatly suppressed with film thickness increasing. Solar-blind ultraviolet photodetector is fabricated based on the β-Ga<sub>2</sub>O<sub>3</sub> film. Its photoelectric detection performances (the photo-to-dark current ratio, responsivity, detectivity, and external quantum efficiency) also increase first and decrease then with the increase of film thickness. The β-Ga<sub>2</sub>O<sub>3</sub> ultraviolet photodetector prepared by a thin film with a thickness of 840 nm exhibits a very low dark current (4.9 × 10<sup>–12</sup> A) under a 5 V bias voltage and an ultraviolet light with a wavelength of 254 nm (600 μW/cm<sup>2</sup>). It exhibits a high photo-to-dark current ratio of 3.2 × 10<sup>5</sup>, and a short response time of 0.09/0.80 s (rising time) and 0.06/0.53 s ratio (falling time). Its responsivity (<i>R</i>), detectivity (<i><u>D</u></i><sup> *</sup>), and the external quantum efficiency (EQE) are 1.19 mA/W, 1.9 × 10<sup>11</sup> Jones, and 0.58%, respectively. The prepared device has quantifiable characteristics, and its photocurrent increases almost linearly with the increase of applied voltage and optical power density, and therefore can work in a linear dynamic region, which indicates that it is very suitable for fabricating the solar-blind ultra-violet detectors.

Highlights

  • The insets are the enlarged view of the relationship between dark s current and voltage. (b), (d), (f) Logarithmic graphs of photo and dark current of device A, D and E, respectively

  • Gao Yue (School of Physics and Electronic Technology, Liaoning Normal University, Dalian 116029, China) ( Received 18 September 2021; revised manuscript received 11 November 2021 )

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Summary

Gauss fit peaks

图 4 (a) 不同薄膜厚度的 b-Ga2O3 薄膜的 PL 光谱; (b) 薄膜厚度约为 840 nm 的 Ga2O3 薄膜的 PL 高斯拟合峰; (c)—(f) 分别显 示了不同厚度 Ga2O3 薄膜在波长约为 378, 415, 456 和 511 nm 处的 PL 拟合峰. 先用掩膜板确定肖特基接触区域的叉指图形, 利用离子溅射仪在制备好的薄膜上溅射一层叉指 形状铂层作为电极, 从而形成肖特基接触, 器件结 构如图 5(a) 所示. 用此方法, 基于不同厚度 b-Ga2O3 薄 膜 (约 210, 420, 630, 840 和 1050 nm) 制 备 了 5 个 MSM 紫外光电探测器, 分别记为器件 A, B, C, D 和 E. 用于构建光电探测器的未掺杂半导体层通 常都会表现出非线性光响应行为, 这种现象可以解 释为由带隙中的复合态中心引起的载流子复合, 因 此, 探究随着时间的推移紫外灯打开和关闭的光响 应就变得尤为重要 [24]. 图 5(b) 给出了器件 A—E 的 I–t 图. 在波长 254 nm(光功率密度 600μW/cm2) 紫外光照射、5 V 偏压下, 可以看出 5 个器件均具 有优异的重复性和稳定性

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