Publication | Closed Access
Real-time effect of electron beam on MoS <sub>2</sub> field-effect transistors
12
Citations
43
References
2020
Year
Irradiation of MoS<sub>2</sub> field-effect transistors (FETs) fabricated on Si/SiO<sub>2</sub> substrates with electron beams (e-beams) below 30 keV creates electron-hole pairs (EHP) in the SiO<sub>2</sub>, which increase the interface trap density (N<sub>it</sub> ) and change the current path in the channel, resulting in performance changes. In situ measurements of the electrical characteristics of the FET performed using a nano-probe system mounted inside a scanning electron microscope show that e-beam irradiation enables both multilayer and monolayer MoS<sub>2</sub> channels act as conductors. The e-beams mostly penetrate the channel owing to their large kinetic energy, while the EHPs formed in the SiO<sub>2</sub> layer can contribute to the conductance by flowing into the MoS<sub>2</sub> channel or inducing the gate bias effect. The analysis of the device parameters in the initial state and the vent-evacuation state after e-beam irradiation can clarify the effect of the interplay between the e-beam-induced EHPs and ambient adsorbates on the carrier behavior, which depends on the thickness of the MoS<sub>2</sub> layer. DC and low frequency noise analysis reveals that the e-beam-induced EHPs increase N<sub>it</sub> from 10<sup>9</sup>-10<sup>10</sup> to 10<sup>11</sup> cm<sup>-2</sup> eV<sup>-1</sup> in both monolayer and multilayer devices, while the interfacial Coulomb scattering parameter α<sub>SC</sub> increases by three times in the monolayer and decreases to one-tenth of its original value in the multilayer. In other words, an MoS<sub>2</sub> layer with a thickness of ∼30 nm is less sensitive to adsorbates by surface screening. Thus, the carrier mobility in the monolayer device decreases from 45.7 to 40 cm<sup>2</sup> V<sup>-1</sup> s<sup>-1</sup>, while in the 30 nm-thick multilayer device, it increases from 4.9 to 5.6 cm<sup>2</sup> V<sup>-1</sup> s<sup>-1</sup>. This is further evidenced by simulations of the distribution of interface traps and channel carriers in the MoS<sub>2</sub> FET before and after e-beam irradiation, demonstrating that Coulomb scattering decreases as the effective channel moves away from the interface.
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