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首页> 外文期刊>Turkish journal of physics >Investigating the effect of self-trapped holes in the current gain mechanism of $ eta mathbf{-}{mathbf{Ga}}_{mathbf{2}}{mathbf{O}}_{mathbf{3}}$ Schottky diode photodetectors
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Investigating the effect of self-trapped holes in the current gain mechanism of $ eta mathbf{-}{mathbf{Ga}}_{mathbf{2}}{mathbf{O}}_{mathbf{3}}$ Schottky diode photodetectors

机译:研究$ beta mathbf { - } { mathbf {ga}} _ { mathbf {ga}} _ { mathbf {}} _ { mathbf {3的效果 $ Schottky Diode PhotoDetectors

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摘要

Monoclinic gallium oxide $(etamathrm{-}{mathrm{Ga}}_{mathrm{2}}{mathrm{O}}_{mathrm{3}})$ has found great research interest in solar blind photodetector (SBP) applications due to its' bandgap $mathrm{sim}$4.85 eV and availability of high quality native crystal growth. Applications including missile guidance, flame detection, underwater/intersatellite communication and water purification systems require SBPs. $etamathrm{-}{mathrm{Ga}}_{mathrm{2}}{mathrm{O}}_{mathrm{3}}$ SBPs with high responsivity values have been published indicating internal gain in these devices. The gain has been attributed to accumulation of self-trapped hole (STH) below Schottky metal which the lowers Schottky barrier in these devices based on some approximations rather than a proper device simulation. In this paper, technology computer-aided design (TCAD) simulation of $etamathrm{-}{mathrm{Ga}}_{mathrm{2}}{mathrm{O}}_{mathrm{3}}$ SBPs are performed to numerically investigate the effect of low hole mobility STHs on Schottky barrier lowering (SBL). The simulations revealed that based on the theoretical hole mobility of $mathrm{1}mathrm{ }mathrm{imes }mathrm{ }{mathrm{10}}^{-mathrm{6}}mathrm{ }{mathrm{cm}}^{mathrm{2}}{mathrm{V}}^{-mathrm{1}}{mathrm{s}}^{-mathrm{1}}$, photoconductive gain in $etamathrm{-}{mathrm{Ga}}_{mathrm{2}}{mathrm{O}}_{mathrm{3}}$ based photodetectors cannot be attributed to STH related hole accumulation near Schottky contact. It is found that hole mobility in the range of $mathrm{1}mathrm{ }mathrm{imes }mathrm{ }{mathrm{10}}^{-mathrm{10}}mathrm{ }{mathrm{cm}}^{mathrm{2}}{mathrm{V}}^{-mathrm{1}}{mathrm{s}}^{-mathrm{1}}mathrm{-}mathrm{ }mathrm{1}mathrm{ }mathrm{imes }mathrm{ }{mathrm{10}}^{-mathrm{12}}mathrm{ }{mathrm{cm}}^{mathrm{2}}{mathrm{V}}^{-mathrm{1}}{mathrm{s}}^{-mathrm{1}}$ is required to induce $mathrm{sim}$0.3 eV of SBL potential. Unless such low hole mobility is reported either experimentally or theoretically, it is not reasonable to attribute gain to STH formation in these devices.
机译:单克镓氧化物$( beta mathrm { - } { mathrm {ga}} _ { mathrm {ga}} { mathrm {}} { mathrm {}} _ { mathrm {3}})$已找到很好的研究兴趣由于其“Bandgap $ Mathrm { SIM}为4.85 eV和高质量的本土水晶增长,因此太阳盲光度探测器(SBP)应用。包括导弹引导,火焰检测,水下/三卫星通信和水净化系统的应用需要SBP。 $ beta mathrm { - } { mathrm {ga}} { mathrm {2}} { mathrm {2}} { mathrm {3}} { mathrm {3}}具有高响应值值的$ sbps已发布,指示内部增益在这些设备中。该增益已归因于肖特基金属下方的自捕集孔(STH)的累积,该孔在这些器件中降低了这些器件中的肖特基势垒基于一些近似而不是适当的设备模拟。在本文中,技术计算机辅助设计(TCAD)仿真$ beta mathrm { - } { mathrm {ga}} _ { mathrm {ga}} { mathrm {}} { mathrm {o}} _ { mathrm {3以$ SBPS进行数值上研究低孔迁移率STH对肖特基屏障降低(SBL)的影响。仿真显示,基于$ mathrm {1} mathrm { mathrm { mathrm { times} mathrm { mathrm { mathrm { mathrm {}} ^ { - mathrm {6}} mathrm {} { mathrm {cm}} { mathrm {v}} { mathrm {v}} { mathrm {1}} { mathrm {s}} ^ { - mathrm {1} $,$ beta mathrm { - } { mathrm {ga}} _ { mathrm {2}} _ { mathrm {}} _ { mathrm {o}}。到肖特基接触附近的STH相关孔积累。发现在$ mathrm {1} mathrm { mathrm { time} mathrm { mathrm { mathrm {} { mathrm {10}} ^ { - mathrm {10}} mathrm中的空穴移动性{ mathrm {cm}} { mathrm {v}} { mathrm {v}} { mathrm {s}} { mathrm {s}} ^ { - mathrm {1}} mathrm { - } mathrm {} mathrm {1} mathrm {} mathrm {} mathrm { time} mathrm {} mathrm {} { mathrm {10}} ^ { - mathrm {12}} mathrm { } { mathrm {cm}} { mathrm {2}} { mathrm {v}} { - mathrm {1}} { mathrm {s}} { mathrm {s}} ^ { - mathrm {1}} $需要诱导$ mathrm { sim} $ 0.3的SBL潜力。除非在实验或理论上报告这种低孔流动性,否则在这些设备中将增益属于STH形成是不合理的。

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