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Traps in MOCVD n-GaN Studied by Deep Level Transient Spectroscopy and Minority Carrier Transient Spectroscopy

机译:深度瞬态透射光谱和少数载体瞬态光谱研究的MOCVD N-GAN中的陷阱

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Electron and hole traps in MOCVD n-GaN have been studied using deep level transient spectroscopy (DLTS) and minority carrier transient spectroscopy (MCTS). Sidoped GaN is grown on sapphire, free-standing n~+-GaN and SiC substrates. DLTS and MCTS measurements are performed for Schottky diodes, p+n diodes and MOS structures. A total of nine electron traps are found in the trap energy depth ranging from 0.24 to 1.2 eV with the trap concentration ranging from 10~(12) to 10~(16) cm~(-3), while a total of five hole traps in the trap energy depth from 0.25 to 1.8 eV with the trap concentration from 10~(14) to 10~(16) cm~(-3). The variation of trap concentrations are discussed in relation to the substrates used. Interface state densities around 1012 cm~(-2)eV~(-1) are obtained for MOS structures on sapphire and n~+-GaN substrates. In carbon-doped n-GaN on SiC, a hole trap with the energy depth of 0.86 eV is observed with the trap concentrations around 1016 cm~(-3), suggesting that this hole trap is carbonrelated. Moreover, a trap with the energy depth of 0.88 eV is detected in high resistivity GaN doped with carbon using optical current DLTS. It is found that traps with the energy levels at Ec-0.57 and Ev+0.86 eV have larger trap concentrations in MOCVD n-GaN, while a trap at Ev+0.86 eV is dominant in carbon-doped n-GaN.
机译:使用深水平瞬态光谱(DLT)和少数型载体瞬态光谱(MCT)研究了MOCVD N-GaN中的电子和孔陷阱。侧身甘地在蓝宝石上生长,独立的N〜+ - 以SIC基板。为肖特基二极管,P + N二极管和MOS结构执行DLT和MCTS测量。在陷阱能量深度范围为0.24至1.2eV的陷阱能量深度,陷阱浓度范围为10〜(12)至10〜(16)厘米〜(-3),总共陷入困境,总共五个孔陷阱在陷阱能量深度为0.25至1.8eV,捕集浓度为10〜(14)至10〜(16)cm〜(-3)。捕获捕集浓度的变异是关于所用基材的讨论的。接口状态密度约为1012cm〜(-2)EV〜(-1),用于Sapphire上的MOS结构和N〜+ -GAN底板。在SiC上的碳掺杂的N-GaN中,通过约1016cm〜(-3)的捕集浓度观察到具有0.86eV的能量深度的空穴阱,表明该孔阱是Carbanderated。此外,在使用光电流DLT的高电阻率GaN中检测具有0.88eV的能量深度的陷阱。发现具有EC-0.57和EV + 0.86eV的能量水平的陷阱在MOCVD N-GaN中具有较大的捕获浓度,而EV + 0.86eV的捕集器在碳掺杂N-GaN中占主导地位。

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