SEMICONDUCTOR DEVICES

Line-edge roughness induced single event transient variation in SOI FinFETs

Weikang Wu, Xia An, Xiaobo Jiang, Yehua Chen, Jingjing Liu, Xing Zhang and Ru Huang

+ Author Affiliations

 Corresponding author: An Xia, Email: anxia@ime.pku.edu.cn; Huang Ru, Email: ruhuang@pku.edu.cn

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Abstract: The impact of process induced variation on the response of SOI FinFET to heavy ion irradiation is studied through 3-D TCAD simulation for the first time. When FinFET biased at OFF state configuration (Vgs=0, Vds=Vdd) is struck by a heavy ion, the drain collects ionizing charges under the electric field and a current pulse (single event transient, SET) is consequently formed. The results reveal that with the presence of line-edge roughness (LER), which is one of the major variation sources in nano-scale FinFETs, the device-to-device variation in terms of SET is observed. In this study, three types of LER are considered: type A has symmetric fin edges, type B has irrelevant fin edges and type C has parallel fin edges. The results show that type A devices have the largest SET variation while type C devices have the smallest variation. Further, the impact of the two main LER parameters, correlation length and root mean square amplitude, on SET variation is discussed as well. The results indicate that variation may be a concern in radiation effects with the down scaling of feature size.

Key words: heavy ion irradiationsingle event transientvariationline-edge roughnessSOIFinFET



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Fig. 1.  Simulated and measured transfer characteristics of SOI FinFET. The experimental data are from Reference [17].

Fig. 2.  (Color online) Comparison of SET in devices with (black lines) and without (red circle) LER. Each curve represents one device. Qcoll is calculated by the integral of SET current. (a) SET. (b) Total collected charge.

Fig. 3.  The electrostatic potential along the center of the fin versus time and (the inset shows) density of ionized electron-hole pairs from top view of the ideal device.

Fig. 4.  (Color online) Device-to-device variation of Qcoll under the presence of LER. The fin volume and electrostatic potential changes from device to device.

Fig. 5.  (a) Distribution of Qcoll corresponding to three types of LER. (b) Calculated variation and normalized deviation. $\mu$ is the average value of Qcoll.

Fig. 6.  Distribution and variation of Qcoll as a function of $\Delta$.

Fig. 7.  (a) Distribution of Qcoll in type A devices. (b) Top view of the fin schematics of the best case and the worst case devices with different $\Delta$. (c) Electrostatic potential variation as a function of $\Delta$s.

Fig. 8.  Distribution and variation of Qcoll as a function of $\Lambda$.

Fig. 9.  (a) Top view of the fin schematics of the best case and the worst case devices with different $\Lambda$. (b) Electrostatic potential variation as a function of $\Lambda$.

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    Received: 11 June 2015 Revised: Online: Published: 01 November 2015

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      Weikang Wu, Xia An, Xiaobo Jiang, Yehua Chen, Jingjing Liu, Xing Zhang, Ru Huang. Line-edge roughness induced single event transient variation in SOI FinFETs[J]. Journal of Semiconductors, 2015, 36(11): 114001. doi: 10.1088/1674-4926/36/11/114001 W K Wu, X An, X B Jiang, Y H Chen, J J Liu, X Zhang, R Huang. Line-edge roughness induced single event transient variation in SOI FinFETs[J]. J. Semicond., 2015, 36(11): 114001. doi: 10.1088/1674-4926/36/11/114001.Export: BibTex EndNote
      Citation:
      Weikang Wu, Xia An, Xiaobo Jiang, Yehua Chen, Jingjing Liu, Xing Zhang, Ru Huang. Line-edge roughness induced single event transient variation in SOI FinFETs[J]. Journal of Semiconductors, 2015, 36(11): 114001. doi: 10.1088/1674-4926/36/11/114001

      W K Wu, X An, X B Jiang, Y H Chen, J J Liu, X Zhang, R Huang. Line-edge roughness induced single event transient variation in SOI FinFETs[J]. J. Semicond., 2015, 36(11): 114001. doi: 10.1088/1674-4926/36/11/114001.
      Export: BibTex EndNote

      Line-edge roughness induced single event transient variation in SOI FinFETs

      doi: 10.1088/1674-4926/36/11/114001
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