Kaiyue He, Zhanqi Li, Taotao Li, Yifu Sun, Shitong Zhu, Chao Wu, Huiping Zhu, Peng Lu, Xinran Wang, Maguang Zhu. Displacement damage effects in MoS2-based electronics[J]. Journal of Semiconductors, 2024, 45(12): 122701

Search by keywords or author
- Journal of Semiconductors
- Vol. 45, Issue 12, 122701 (2024)

Fig. 1. (Color online) Characterization of a CVD-grown monolayer MoS2 film. (a) Schematic presentation of the seeding-promoted CVD with a customized inner reactor for the synthesis of monolayer MoS2. (b) and (c) Line scan of Raman spectra and PL spectra of the monolayer MoS2 film, performed in this study with a 488 nm laser. (d) A schematic diagram and process flow detailing the device structure are provided. A 285 nm SiO2 layer serves as the gate dielectric in this design. (e) Transfer characteristics of 20 MoS2 FETs with L = 3 μm and W = 4 μm, under Vds = 3 V. (f) Corresponding output characteristics of the MoS2 FET. Vgs is stepped up from −12 to 30 V by increments of 3 V.

Fig. 2. (Color online) Raman analysis of the MoS2 FETs before and after 30 keV proton irradiation. (a) Raman spectra of monolayer MoS2 analysis under different proton fluence. (b) Position of and in correlation with the proton fluence. The peak position's error bars represent the largest uncertainty present. (c) The peak-to-peak distance and (d) peak intensity ratio for the Raman spectra were measured at 30 different locations within a 5 μm by 6 μm area before irradiation. Insets in the upper right corner of the color maps show the mean (μ) and standard deviation (σ) for each parameter. (e) The peak-to-peak distance and (f) peak intensity ratio for the Raman spectra at the same points after irradiation with a fluence of 1014 p/cm2.

Fig. 3. (Color online) Electrical performance of the MoS2 FETs before and after 30 keV proton irradiation. (a) A diagrammatic representation of the DD effect in the MoS2 FET caused by proton irradiation. Representative transfer characteristics obtained from 20 monolayer MoS2 FETs after proton irradiation with a total fluence of (b) 1012 p/cm2, (c) 1013 p/cm2, and (d) 1014 p/cm2. Statistical measurements of (e) SS, (f) Ion/Ioff, and (g) Vth change, with three different proton irradiation fluences of 1012, 1013, and 1014 p/cm2.
![(Color online) The relationship between radiation absorption cross-section and radiation tolerance. (a) Simulation results of the vacancy number in the source/drain region (Sb/Au/MoS2/SiO2/Si) by SRIM. Inset illustrates the simulation domain, encompassing the source/drain contact region. (b) Simulation results of vacancies number in the monolayer, bilayer and trilayer by SRIM. Transfer characteristics of (c) bilayer and (d) trilayer MoS2 FETs after 1014 p/cm2 proton irradiation measured at different Vds. Benchmark of the change of (e) ΔSS and (f) ΔVth caused by DD in other radiation-hard FETs[11, 20, 21, 35−39].](/Images/icon/loading.gif)
Fig. 4. (Color online) The relationship between radiation absorption cross-section and radiation tolerance. (a) Simulation results of the vacancy number in the source/drain region (Sb/Au/MoS2/SiO2/Si) by SRIM. Inset illustrates the simulation domain, encompassing the source/drain contact region. (b) Simulation results of vacancies number in the monolayer, bilayer and trilayer by SRIM. Transfer characteristics of (c) bilayer and (d) trilayer MoS2 FETs after 1014 p/cm2 proton irradiation measured at different Vds. Benchmark of the change of (e) ΔSS and (f) ΔVth caused by DD in other radiation-hard FETs[11, 20, 21, 35−39].

Set citation alerts for the article
Please enter your email address