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Radiation sustenance of HfO_2/β-Ga_2O_3 metal-oxide-semiconductor capacitors: gamma irradiation study

机译:HFO_2 /β-GA_2O_3金属氧化物半导体电容器的辐射寄托:伽马辐射研究

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摘要

beta-Ga2O3 is an interesting new generation wide bandgap semiconductor for power device applications. The gamma irradiation was performed on the HfO2/beta-Ga2O3-based metal-oxide-semiconductor capacitors at 1 kGy and 200 kGy doses. The leakage current density variation at -1 V is 3.47 x 10(-7) A cm(-2), 5.90 x 10(-7) A cm(-2) and 4.91 x 10(-6) A cm(-2) for the pristine, 1 kGy and 200 kGy devices, respectively. In the case of substrate injection, the Schottky emission mechanism appears to be dominant in the 0.65 to 2.0 MV cm(-1) electric field range. The barrier heights (Ni/HfO2/beta-Ga2O3) 0.95 eV, 0.86 eV and 0.83 eV were extracted from Schottky emission for the pristine, 1 kGy and 200 kGy doses, respectively. However, as the dose increases to 200 kGy, the charge-trapping favors the trap-assisted Poole-Frenkel (PF) tunneling mechanism. In this case, the PF emission mechanism seems to be dominant for the pristine and 1 kGy in the range of 2.0-4.0 MV cm(-1), whereas for 200 kGy it is 1.45 to 4.0 MV cm(-1) which indicates that the defect assisted PF tunneling is predominant at 200 kGy irradiation dose. There is an increase in the density of oxide traps (D-ot) changes from 1.14 x 10(12) cm(-2) eV(-1) to 1.47 x 10(12) cm(-2) eV(-1), and the density of interface traps has increased from 1.95 x 10(11) cm(-2) eV(-1) to 3.80 x 10(11) cm(-2) eV(-1) for the pristine and 200 kGy samples, respectively. The peaks of Photoluminescence show that the three bands of defects centered at 3.0, 2.7 and 2.2 eV. These peaks have possibly arisen from the vacancies of oxygen. At 200 kGy high dose, the defect band emissions were found at 2.9, 2.6 eV and a broad emission at 2.1 eV indicates the increase in the denisty of oxide-trapped charges within the HfO2 layer.
机译:Beta-Ga2O3是一种有趣的新一代宽带隙半导体,用于电力设备应用。在1 kgy和200kgy剂量上对基于HFO2 /β-GA2O3的金属氧化物 - 半导体电容进行γ辐射。 -1V的漏电流密度变化为3.47×10(-7)厘米(-2),5.90×10(-7)A cm(-2)和4.91×10(-6)厘米(-2 )对于原始,1 kgy和200 kgy设备。在基板注射的情况下,肖特基排放机构似乎在0.65至2.0mVcm(-1)电场范围内占主导地位。屏障高度(Ni / HFO2 /β-GA2O3)0.95eV,0.86eV和0.83eV分别从肖特基排放分别为原始,1kGy和200kgy剂量提取。然而,随着剂量增加到200 kgy,电荷捕获有利于陷阱辅助普尔弗雷克尔(PF)隧道机构。在这种情况下,PF排放机制似乎对原始和1kGy的主要占优势在2.0-4.0 mV cm(-1)的范围内,而200 kgy为1.45至4.0 mV cm(-1),表示这一点缺陷辅助PF隧道在200吨杆照射剂量上是主要的。氧化物疏水阀(D-OT)的密度增加到1.14×10(12)cm(-2)eV(-1)至1.47×10(12)cm(-2)EV(-1) ,界面捕集物的密度从1.95×10(11)厘米(-2)厘米(-2)厘米(-1)厘米到3.80×10(11)厘米(-2)EV(-1),用于原始和200 kgy样本, 分别。光致发光的峰表明,缺陷的三个带以3.0,2.7和2.2eV为中心。这些峰可能从氧气的空位中出现。在200 kgy高剂量时,缺陷带排放位于2.9,2.6eV和2.1eV的广泛发射,表明HFO2层内氧化物捕获的电荷的增加。

著录项

  • 来源
    《Semiconductor science and technology》 |2020年第5期|055024.1-055024.7|共7页
  • 作者单位

    Indira Gandhi Ctr Atom Res Mat Sci Grp Kalpakkam 603102 Tamil Nadu India;

    Indian Inst Technol Delhi Dept Phys Hauz Khas New Delhi 110016 India;

    Indira Gandhi Ctr Atom Res MMG Nondestruct Evaluat Div Kalpakkam 603102 Tamil Nadu India;

    Indian Inst Technol Delhi Dept Phys Hauz Khas New Delhi 110016 India;

    Indira Gandhi Ctr Atom Res Mat Sci Grp Kalpakkam 603102 Tamil Nadu India|Indira Gandhi Ctr Atom Res Elect & Instrumentat Grp Kalpakkam 603102 Tamil Nadu India;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

    beta-Ga2O3; gamma irradiation; high-k dielectrics; HfO2; beta-Ga2O3; MOS capacitors; radiation hardness;

    机译:Beta-Ga2O3;伽玛辐射;高k电介质;HFO2;BETA-GA2O3;MOS电容器;辐射硬度;
  • 入库时间 2022-08-18 21:19:53

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