Border-Trap Characterization for Ge Gate Stacks Using Deep-Level Transient Spectroscopy

Border-Trap Characterization for Ge Gate Stacks Using Deep-Level Transient Spectroscopy
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使用深能级瞬态光谱对 Ge 栅极堆栈进行边界陷阱表征

DOI:
10.1149/09204.0003ecst
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发表时间:
2019
期刊:
ECS transactions
影响因子:
--
通讯作者:
Dong Wang
Dong Wang
中科院分区:
--
文献类型:
--
作者:
Hiroshi Nakashima;Wei-Chen Wen;Keisuke Yamamoto;Dong Wang

文献摘要

相似文献

利用带锁定积分器的深能级暂态光谱技术,建立了一种对SiO_2/GeO_2/Ge栅堆栈边界陷阱(BT)的评价方法。采用后钝化热氧化工艺制备了具有SiO_2/GeO_2/Ge栅层的Ge金属氧化物半导体电容器(MOSCAP)。基于界面陷阱(IT)和BT信号对注入脉冲强度的不同依赖关系,成功地分离了IT和BT信号。利用p型MOSCAP测量了GeO2/Ge界面0.4 nm处的BTS。这些势垒的能量集中在Ge价带边附近,密度(NBT)在1017-1018 cm−3之间。这些BTS的能量分布在Ge的导带边缘附近较宽的范围内,NBT大约比p-MOSCAP高一个数量级。我们还发现,Al后金属化退火可以钝化靠近Ge价带边的ITS和BTS,但不能钝化靠近导带边缘的ITS和BTS。
A border trap (BT) evaluation method was established for SiO2/GeO2/Ge gate stacks by using deep-level transient spectroscopy with a lock-in integrator. Ge metal-oxidesemiconductor capacitors (MOSCAPs) with SiO2/GeO2/Ge gate stacks were fabricated by post-passivation thermal oxidation. The interface trap (IT) and BT signals were successfully separated based on their different dependences on the intensity of injection pulses. By using p-type MOSCAPs, BTs at the position of 0.4 nm from GeO2/Ge interface were measured. The energy of these BTs was centralized at the position near to the valence band edge of Ge, and the density (Nbt) was in the range of 1017-1018 cm− 3. For n-type MOSCAPs, BTs at the position range of 2.8-3.4 nm from the GeO2/Ge interface were measured. The energy of these BTs were distributed in a relatively wide range near to the conduction band edge of Ge, and the Nbt was approximately one order of magnitude higher than those for p-MOSCAPs. We also found that Al post metallization annealing can passivate both ITs and BTs near to the valence band edge of Ge but not those near to the conduction band edge.