2020
DOI: 10.1016/j.apsusc.2020.146656
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On the origin of the premature breakdown of thermal oxide on 3C-SiC probed by electrical scanning probe microscopy

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Cited by 10 publications
(9 citation statements)
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“…Both samples provide C-V curves negatively shifted compared to the ideal value VFB = +0.9 V. In particular, the experimental flat band voltage values were −0.6 V and −3 V for the T-ALD and PE-ALD stacks, respectively. However, as can be observed in Figure 2c, such negative shifts were smaller compared to that of MOS capacitor where the insulator was only a thick (40 nm) thermal SiO2 [37]. This experimental finding is related to the higher dielectric constant of the Al2O3 (κ = 8) with respect to that Lateral MOS capacitors schematically depicted in Figure 2a were fabricated using photolithography, metal deposition and lift-off processes.…”
Section: Discussionmentioning
confidence: 80%
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“…Both samples provide C-V curves negatively shifted compared to the ideal value VFB = +0.9 V. In particular, the experimental flat band voltage values were −0.6 V and −3 V for the T-ALD and PE-ALD stacks, respectively. However, as can be observed in Figure 2c, such negative shifts were smaller compared to that of MOS capacitor where the insulator was only a thick (40 nm) thermal SiO2 [37]. This experimental finding is related to the higher dielectric constant of the Al2O3 (κ = 8) with respect to that Lateral MOS capacitors schematically depicted in Figure 2a were fabricated using photolithography, metal deposition and lift-off processes.…”
Section: Discussionmentioning
confidence: 80%
“…The MOS structures fabricated on T-Al 2 O 3 /SiO 2 /3C-SiC and PE-Al 2 O 3 /SiO 2 /3C-SiC were probed by C-V measurements, which are shown in Figure 2 c. Both samples provide C-V curves negatively shifted compared to the ideal value V FB = +0.9 V. In particular, the experimental flat band voltage values were −0.6 V and −3 V for the T-ALD and PE-ALD stacks, respectively. However, as can be observed in Figure 2 c, such negative shifts were smaller compared to that of MOS capacitor where the insulator was only a thick (40 nm) thermal SiO 2 [ 37 ]. This experimental finding is related to the higher dielectric constant of the Al 2 O 3 (κ = 8) with respect to that of SiO 2 (κ = 3.9).…”
Section: Discussionmentioning
confidence: 98%
“…[25] In general, gate J g with a sudden jump exceeding 3 orders can be regarded as hard breakdown. [26] The soft breakdown part is the area where the J g increases obviously without hard breakdown, and the electric field of gate oxide (E ox ) from 6 MV/cm to the intrinsic breakdown field (E int ) is the soft breakdown part. The gate oxide is tested by TDDB with constant stress electric field (E str ) which is determined by TZDB test.…”
Section: Resultsmentioning
confidence: 99%
“…Besides the application on Schottky contacts described in Section 3.1 , nanoscale resolution current mapping by C-AFM can also be a powerful analysis technique for investigation of the dielectric breakdown behaviour of thin insulators. In fact, this method was recently employed by Fiorenza et al [ 79 ] in order to explain the reasons behind the premature breakdown of thermal oxide (SiO 2 ) grown on 3C-SiC typically observed in MOS capacitors, by stressing the oxide through the application of a bias to the C-AFM tip corresponding to an electric field of 8 MV/cm (see schematic set-up in Figure 10 a).…”
Section: Processing Technology For 3c-sicmentioning
confidence: 99%