2021
DOI: 10.1016/j.jallcom.2021.158895
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Determination of scattering mechanisms in AlInGaN/GaN heterostructures grown on sapphire substrate

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Cited by 9 publications
(6 citation statements)
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“…where R sh is intrinsically determined by the electric conductivity of 2DEG; and n s and µ N denote the electrical parameters of 2DEG. This finding reveals that n s and µ N are related to the polarisation effect and roughness scatterings caused by alloys of the (In)Al(Ga)N/GaN heterojunction [106,166]. Currently, the (In)Al(Ga)N/GaN heterojunction of GaNbased HEMTs includes AlGaN/GaN, InAlN/GaN, AlN/GaN, GaN/AlN SL barrier layers and multi-channel AlGaN/GaN layers [167][168][169][170][171][172].…”
Section: (In)al(ga)n/gan Heterojunctionmentioning
confidence: 84%
“…where R sh is intrinsically determined by the electric conductivity of 2DEG; and n s and µ N denote the electrical parameters of 2DEG. This finding reveals that n s and µ N are related to the polarisation effect and roughness scatterings caused by alloys of the (In)Al(Ga)N/GaN heterojunction [106,166]. Currently, the (In)Al(Ga)N/GaN heterojunction of GaNbased HEMTs includes AlGaN/GaN, InAlN/GaN, AlN/GaN, GaN/AlN SL barrier layers and multi-channel AlGaN/GaN layers [167][168][169][170][171][172].…”
Section: (In)al(ga)n/gan Heterojunctionmentioning
confidence: 84%
“…Figure 12c demonstrates the Hall mobility µ H of the SrPb 3 Br 8 sample at 110–300 K. The Hall mobility µ H of SrPb 3 Br 8 is 0.13594 cm 2 V −1 s −1 at 110 K, and it declines as the temperature increases, reaching 0.02363 cm 2 V −1 s −1 at 300 K. The scattering mechanism in the crystal has a direct impact on µ H , including ionized impurity scattering, lattice vibration scattering (acoustic wave scattering and optical wave scattering). [ 30 ] In most cases, the main scattering mechanisms necessarily considered are ionized impurity scattering and acoustic wave scattering. Their effect on mobility can be expressed as follows: μiNi1T32$$\begin{equation}{\mu }_{\rm{i}} \propto N_{\rm{i}}^{ - 1}{T}^{\frac{3}{2}}\end{equation}$$ μST32$$\begin{equation}{\mu }_{\rm{S}} \propto {T}^{ - \frac{3}{2}}\end{equation}$$where N i represents the concentration of ionized impurity.…”
Section: Resultsmentioning
confidence: 99%
“…One novel approach, initially suggested by Ketteniss et al and subsequently confirmed, involves using a thin quaternary AlInGaN barrier layer that introduces polarization engineering between the barrier and the GaN channel, enabling E-mode operation [11,12]. Quaternary nitride has garnered significant attention as an alternative to AlGaN barrier layers due to its promising DC and RF performance, including the ability to utilize high aluminum content, leading to increased spontaneous polarization induced by high 2DEG carrier density (ns > ~1.8×10 13 cm -2 ) and high mobility (µ > ~ 1800 cm 2 /V s) [13][14][15]. Traditionally, since 1991, HEMT transistors have been designed and fabricated with a single barrier layer [16].…”
Section: Introductionmentioning
confidence: 99%