2012
DOI: 10.1016/j.matchemphys.2012.01.128
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Effects of growth conditions on the acceptor activation of Mg-doped p-GaN

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Cited by 29 publications
(12 citation statements)
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“…Because GaN material has aa negative differential mobility effect, a lower electric field can make the electrons in GaN material reach higher drift velocity. According to IMPATT current Equation (7), νs is the average drift velocity that carriers can reach in a semiconductor device, which explains why SiC/GaN IMPATT has a higher rf output current and frequency bandwidth. In a word, the rf electric field in the drift region can obtain a larger swing to achieve a lower value, and this electric field modulation is another mechanism to improve the performance of SiC/GaN IMPATT.…”
Section: Large-signal Simulation Results and Discussionmentioning
confidence: 99%
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“…Because GaN material has aa negative differential mobility effect, a lower electric field can make the electrons in GaN material reach higher drift velocity. According to IMPATT current Equation (7), νs is the average drift velocity that carriers can reach in a semiconductor device, which explains why SiC/GaN IMPATT has a higher rf output current and frequency bandwidth. In a word, the rf electric field in the drift region can obtain a larger swing to achieve a lower value, and this electric field modulation is another mechanism to improve the performance of SiC/GaN IMPATT.…”
Section: Large-signal Simulation Results and Discussionmentioning
confidence: 99%
“…Before the rf power of IMPATT reaches saturation, it increases with the p-region concentration [5,6]. However, the practical fabrication of p-n junction GaN structures is challenging in IMPATT devices due to the difficulty of obtaining high concentrations of p-GaN because of the very low effective hole ionization rate [7]. Eventually, the voltage and current of this negative resistance device will be reduced, impairing the diode performance severely [8].…”
Section: Introductionmentioning
confidence: 99%
“…In addition, the WPE of LED sample C demonstrated a 3.5% improvement in comparison with that of LED sample B, which is mainly attributed to the lower forward voltage of LED sample C. The Hall effect and x-ray photoemission spectroscopy (XPS) measurements were carried out in the following experiment to explain the improved performance for LED sample C. In order to clarify the mechanism of activation of p-type GaN at a relatively low temperature of 500°C in N 2 ambient, p-type GaN epitaxial wafers without MQWs active region were grown by MOCVD as follows: The epitaxial layers were done by sequentially depositing of a 30-nm-thick low-temperature GaN nucleation layer, a 2.0-μm-thick undoped GaN layer, a 0.6-μm-thick p-type GaN layer, and a 2.0-nm-thick InGaN strained layer on sapphire substrates. X-ray rocking curves showed that the full width at half maximums of the wafers was 299 arcsec for (0002) symmetric plane, indicating a good quality of the p-type GaN layers [ 21 ]. A 100-nm-thick ITO film was evaporated on the p-type GaN epitaxial layers by the electron beam evaporator.…”
Section: Resultsmentioning
confidence: 99%
“…However, owing to the difficulty in the doping manufacturing process of p-GaN, a high-concentration of ionized holes cannot be formed [ 14 ], leading to a series of problems. Firstly, because of the overly low p-type region concentration and poor mobility characteristics, the electric field distribution in the avalanche region deviates from the ideal situation, deteriorating the impact-ionzation characteristics and inducing the device performance to decline.…”
Section: Introductionmentioning
confidence: 99%