赵洪利, 高林春, 曾传滨, 刘魁勇, 罗家俊, 韩郑生. DCIV技术提取SOI器件前栅界面与背界面态密度[J]. 微电子学与计算机, 2015, 32(6): 82-84,89. DOI: 10.19304/j.cnki.issn1000-7180.2015.06.018
引用本文: 赵洪利, 高林春, 曾传滨, 刘魁勇, 罗家俊, 韩郑生. DCIV技术提取SOI器件前栅界面与背界面态密度[J]. 微电子学与计算机, 2015, 32(6): 82-84,89. DOI: 10.19304/j.cnki.issn1000-7180.2015.06.018
ZHAO Hong-li, GAO Lin-chun, ZENG Chuan-bin, LIU Kui-yong, LUO Jia-jun, HAN Zheng-sheng. DCIV Technique for Extracting Front Channel and Back Channel Interface Traps Density in SOI Device[J]. Microelectronics & Computer, 2015, 32(6): 82-84,89. DOI: 10.19304/j.cnki.issn1000-7180.2015.06.018
Citation: ZHAO Hong-li, GAO Lin-chun, ZENG Chuan-bin, LIU Kui-yong, LUO Jia-jun, HAN Zheng-sheng. DCIV Technique for Extracting Front Channel and Back Channel Interface Traps Density in SOI Device[J]. Microelectronics & Computer, 2015, 32(6): 82-84,89. DOI: 10.19304/j.cnki.issn1000-7180.2015.06.018

DCIV技术提取SOI器件前栅界面与背界面态密度

DCIV Technique for Extracting Front Channel and Back Channel Interface Traps Density in SOI Device

  • 摘要: 直流电流电压(DCIV)方法不仅可以提取SOI器件前栅沟道界面态密度,也可应用于背界面态密度的提取.给出了具体的测试步骤与方法,以0.13 μm SOI工艺制造的NMOS器件为测试对象,对前栅界面与背界面分别进行了测试.基于DCIV理论,将实验得到的界面复合电流值与理论公式做最小二乘拟合,不仅获得了各界面态密度,也得到界面态密度所在的等效能级.结果表明,采用了智能剥离技术制备的SOI NMOS器件背界面态密度量级为1010cm-2,前栅界面的态密度小于背界面的,量级为109cm-2,并给出了两界面态面密度所在的等效能级.

     

    Abstract: Direct Current Current Voltage(DCIV) technique can extract not only the front channel interface traps but also the back channel interface traps. The concrete steps and methods is presented and is applied to measure the front channel interface and the back channel interface traps in SOI NMOSFET which is fabricated in 0.13 μm technologie. On the basis of the DCIV theory, the interface recombination current obtained can be used to fit the theoretical equation with least-squares optimization, then both the interface trap density and its equivalent energy can be acquired. The results indicate that the back channel interface trap density of SOI NMOSFET adopting SMRT-CUT technique are larger than 1010cm-2,and the front channel interface trap density is smaller than the back channel interfaces'. The corresponding interface trap density equivalent energy is also presented.

     

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