2014
DOI: 10.1016/j.sse.2013.09.009
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Modeling of sheet carrier density and microwave frequency characteristics in Spacer based AlGaN/AlN/GaN HEMT devices

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Cited by 36 publications
(32 citation statements)
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“…Figure shows the variation of transconductance g m for the B‐doped GaN cap DH‐HEMT devices with x = 0%, 1%, 3%, 5%, and 7% at V ds = 15 V. The peak g m is 0.182 S/mm, 0.179 S/mm, 0.176 S/mm, 0.15 S/mm, and 0.127 S/mm for the GaN, Al 0.01 Ga 0.99 N, Al 0.03 Ga 0.97 N, Al 0.05 Ga 0.95 N, and Al 0.07 Ga 0.93 N back‐barrier/buffers, respectively. g m is a very important figure of merit for a device and larger the g m , greater is the gain . The decrease in I ds,sat and peak g m of AlGaN DH‐HEMTs is due to the lower density of 2DEG in the channel …”
Section: Resultsmentioning
confidence: 99%
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“…Figure shows the variation of transconductance g m for the B‐doped GaN cap DH‐HEMT devices with x = 0%, 1%, 3%, 5%, and 7% at V ds = 15 V. The peak g m is 0.182 S/mm, 0.179 S/mm, 0.176 S/mm, 0.15 S/mm, and 0.127 S/mm for the GaN, Al 0.01 Ga 0.99 N, Al 0.03 Ga 0.97 N, Al 0.05 Ga 0.95 N, and Al 0.07 Ga 0.93 N back‐barrier/buffers, respectively. g m is a very important figure of merit for a device and larger the g m , greater is the gain . The decrease in I ds,sat and peak g m of AlGaN DH‐HEMTs is due to the lower density of 2DEG in the channel …”
Section: Resultsmentioning
confidence: 99%
“…g m is a very important figure of merit for a device and larger the g m , greater is the gain. 29 The decrease in I ds,sat and peak g m of AlGaN DH-HEMTs is due to the lower density of 2DEG in the channel. 28 Figure 9 shows the comparison and variation of I ds,sat and g m values for B-doped and Mg-doped GaN cap DH-HEMT extracted from I ds -V gs transfer characteristics of the devices for various Al content "x" in Al x Ga 1-x N back-barrier/buffer.…”
Section: Resultsmentioning
confidence: 99%
“…where N i = (n s p s ) 0.5 . The various bound elements in the mobility model 24 are as follows: a = 2.61 × 10 −4 V s cm −2 , b = 2.9 × 10 −4 V s cm −2 , and c = 1.7 × 10 −2 V s cm −2 .…”
Section: Mobility Modelmentioning
confidence: 99%
“…Introduction of AlN binary layer in AlGaN/GaN and AlInN/GaN material system results in high polarization-induced sheet charge density at the heterointerface due to large polarization charges and conduction band offset. 10,12 The 2-dimensional electron gas (2DEG) mobility increases due to less alloy disorder scattering 13,14 and reduction of the electron-wave penetration into the AlGaN or AlInN barrier layer. 12 To achieve better performance, the aspect ratio of the device is the vital factor that influences the device operation.…”
Section: Introductionmentioning
confidence: 99%
“…10,12 The 2-dimensional electron gas (2DEG) mobility increases due to less alloy disorder scattering 13,14 and reduction of the electron-wave penetration into the AlGaN or AlInN barrier layer. 12 To achieve better performance, the aspect ratio of the device is the vital factor that influences the device operation. Therefore, the ratio between the gate length (L g ) and the gate-to-channel separation needs to be considered when L g decreases.…”
Section: Introductionmentioning
confidence: 99%