2023
DOI: 10.1088/1674-4926/44/7/072803
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Experimental investigation on the instability for NiO/β-Ga2O3 heterojunction-gate FETs under negative bias stress

Abstract: A NiO/β-Ga2O3 heterojunction-gate field effect transistor (HJ-FET) is fabricated and its instability mechanisms are experimentally investigated under different gate stress voltage (V G,s) and stress times (t s). Two different degradation mechanisms of the devices under negative bias stress (NBS) are identified. At low V G,s for a short t s, NiO bulk traps trapping/de-trapping electrons are responsible for decrease/recovery of the leakage c… Show more

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Cited by 6 publications
(4 citation statements)
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“…To study the electrical instability of the device passivated with HfO 2 , we measured the transfer characteristics under NBS at room temperature, setting the stress time from 0 s to 3600 s. We only interrupted the applied stress for the measurement by quick sweeping V GS from −10 to 0 V. Figure 5(a) shows the shift of the I DS -V GS for V DS = 1 V when a constant bias stress voltage was applied at V GS = −10 V. A performance degradation of g m , SS, and D it was observed, as shown in figures 5(b) and (c), which was attributed to increased electron trapping and de-trapping between gate interface and the channel due to negative gate bias stress [25]. Figure 5(d) shows the change in the extracted ∆V TH as a function of stress time for the HfO 2 −, Al 2 O 3 -passivated, and unpassivated devices, which were cited from our previous result [17,26].…”
Section: Resultsmentioning
confidence: 93%
“…To study the electrical instability of the device passivated with HfO 2 , we measured the transfer characteristics under NBS at room temperature, setting the stress time from 0 s to 3600 s. We only interrupted the applied stress for the measurement by quick sweeping V GS from −10 to 0 V. Figure 5(a) shows the shift of the I DS -V GS for V DS = 1 V when a constant bias stress voltage was applied at V GS = −10 V. A performance degradation of g m , SS, and D it was observed, as shown in figures 5(b) and (c), which was attributed to increased electron trapping and de-trapping between gate interface and the channel due to negative gate bias stress [25]. Figure 5(d) shows the change in the extracted ∆V TH as a function of stress time for the HfO 2 −, Al 2 O 3 -passivated, and unpassivated devices, which were cited from our previous result [17,26].…”
Section: Resultsmentioning
confidence: 93%
“…Monitoring V th shifts and R on under positive bias stress (PBS) and negative bias stress (NBS) can help to identify traps contributing to the FET instability and degradation. This has been studied in recessed-gate [252], p-NiO-gate [253], and β-Ga 2 O 3 /SiC FETs [254]. PBS-induced instability is primarily caused by border traps in the gate oxide, while NBSinduced instability is attributed to both interface states and border traps [252].…”
Section: Characterizationmentioning
confidence: 99%
“…PBS-induced instability is primarily caused by border traps in the gate oxide, while NBSinduced instability is attributed to both interface states and border traps [252]. In p-NiO gated FETs, a high V GS or long stress time permanently negatively shifted the V th by ionizing interface dipoles, which neutralized ionized charges in the depletion region [253].…”
Section: Characterizationmentioning
confidence: 99%
“…According to the conventional single-level SRH model for WBG materials, the rate of nonradiative carrier recombination in these materials should be small. Nevertheless, this is clearly inconsistent with the experimental observations, as many oxides and nitrides exhibit a significant carrier-mediated nonradiative recombination rate. Therefore, the conventional single-level SRH model faces a conundrum when it comes to comprehending the substantial nonradiative recombination rates observed in WBG materials. It is imperative to elucidate new nonradiative recombination mechanisms in these materials.…”
Section: Introductionmentioning
confidence: 99%