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Ir~(4+) ions in β-Ga_2O_3 crystals: An unintentional deep donor

机译:β-Ga_2O_3晶体中的Ir〜(4+)离子:无意的深施主

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摘要

Electron paramagnetic resonance (EPR) and infrared absorption are used to detect Ir4+ ions in beta-Ga2O3 crystals. Mg and Fe doped crystals are investigated, and concentrations of Ir4+ ions greater than 1 x 10(18) cm(-3) are observed. The source of the unintentional deep iridium donors is the crucible used to grow the crystal. In the Mg-doped crystals, the Ir4+ ions provide compensation for the singly ionized Mg acceptors and thus contribute to the difficulties in producing p-type behavior. The Ir4+ ions replace Ga3+ ions at the Ga(2) sites, with the six oxygen neighbors forming a distorted octahedron. A large spin-orbit coupling causes these Ir4+ ions to have a low-spin (5d(5), S = 1/2) ground state. The EPR spectrum consists of one broad line with a significant angular dependence. Principal values of the g matrix are 2.662, 1.815, and 0.541 (with principal axes near the crystal a, b, and c directions, respectively). Ionizing radiation at 77 K decreases the Ir4+ EPR signal in Mg-doped crystals and increases the signal in Fe-doped crystals. In addition to the EPR spectrum, the Ir4+ ions have an infrared absorption band representing a d-d transition within the t(2g) orbitals. At room temperature, this band peaks near 5153 cm(-1) (1.94 mu m) and has a width of 17 cm(-1). The band is highly polarized: its intensity is maximum when the electric field E is parallel to the b direction in the crystal and is nearly zero when E is along the c direction. Published under license by AIP Publishing.
机译:电子顺磁共振(EPR)和红外吸收用于检测β-Ga2O3晶体中的Ir4 +离子。研究了Mg和Fe掺杂的晶体,并观察到Ir4 +离子的浓度大于1 x 10(18)cm(-3)。意外的深铱供体的来源是用来生长晶体的坩埚。在掺Mg的晶体中,Ir4 +离子为单离子化的Mg受体提供了补偿,因此造成了产生p型行为的困难。 Ir4 +离子取代了Ga(2)处的Ga3 +离子,六个氧邻域形成了扭曲的八面体。大的自旋轨道耦合导致这些Ir4 +离子具有低自旋(5d(5),S = 1/2)基态。 EPR谱由一条宽的线组成,具有明显的角度依赖性。 g矩阵的主要值为2.662、1.815和0.541(主轴分别位于晶体a,b和c方向附近)。 77 K的电离辐射会降低掺Mg晶体中的Ir4 + EPR信号,并增加掺Fe晶体中的信号。除EPR谱外,Ir4 +离子还具有代表在t(2g)轨道内d-d跃迁的红外吸收带。在室温下,该谱带在5153 cm(-1)(1.94μm)附近达到峰值,宽度为17 cm(-1)。该带是高度极化的:当电场E平行于晶体中的b方向时,其强度最大,而当E沿c方向时,其强度几乎为零。由AIP Publishing授权发布。

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  • 来源
    《Journal of Applied Physics》 |2019年第4期|045703.1-045703.8|共8页
  • 作者单位

    Air Force Inst Technol, Dept Engn Phys, Wright Patterson AFB, OH 45433 USA;

    Air Force Inst Technol, Dept Engn Phys, Wright Patterson AFB, OH 45433 USA;

    Air Force Inst Technol, Dept Engn Phys, Wright Patterson AFB, OH 45433 USA;

    Air Force Inst Technol, Dept Engn Phys, Wright Patterson AFB, OH 45433 USA;

    West Virginia Univ, Dept Phys & Astron, Morgantown, WV 26506 USA;

    Northrop Grumman Synopt, 1201 Continental Blvd, Charlotte, NC 28273 USA;

    Northrop Grumman Synopt, 1201 Continental Blvd, Charlotte, NC 28273 USA;

    Air Force Res Lab, Sensors Directorate, Wright Patterson AFB, OH 45433 USA;

    Air Force Res Lab, Mat & Mfg Directorate, Wright Patterson AFB, OH 45433 USA;

    Air Force Res Lab, Mat & Mfg Directorate, Wright Patterson AFB, OH 45433 USA;

  • 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);
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