2019
DOI: 10.1039/c9ra03121a
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High-energy proton irradiation damage on two-dimensional hexagonal boron nitride

Abstract: The dielectric layer, which is an essential building block in electronic device circuitry, is subject to intrinsic or induced defects that limit its performance.

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Cited by 2 publications
(2 citation statements)
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“…A high I GS of 8.5 × 10 –7 A was maintained until the termination of the proton beam, when I GS recovered to its original value at the fourth cycle. The increased I GS observed in this study can be attributed to the hopping or tunneling of carriers through the ionized trapping states in the dielectric that were formed via the ionizing radiation dose. , …”
Section: Resultsmentioning
confidence: 99%
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“…A high I GS of 8.5 × 10 –7 A was maintained until the termination of the proton beam, when I GS recovered to its original value at the fourth cycle. The increased I GS observed in this study can be attributed to the hopping or tunneling of carriers through the ionized trapping states in the dielectric that were formed via the ionizing radiation dose. , …”
Section: Resultsmentioning
confidence: 99%
“…The increased I GS observed in this study can be attributed to the hopping or tunneling of carriers through the ionized trapping states in the dielectric that were formed via the ionizing radiation dose. 58,59 In situ measurements of the (4:1:1) ZITO TFT revealed that after the end of proton exposure, the enhanced I DS remains almost unchanged, with the negative-shifted V th recovering only to −68 V for the eighth cycle (Figure 3C and Table S7). Although such in situ degradation could originate from the additional interface-trapped and oxide-trapped charge buildup in the gate dielectric layer, the radiation-induced conductivity increase in the semiconductor layer should not be overlooked.…”
Section: In Situ Irradiation Results For (4:1:1) Zito Tftsmentioning
confidence: 99%