{'fraction_non_alphanumeric': 0.029635901778154106, 'fraction_numerical': 0.01947502116850127, 'mean_word_length': 4.372727272727273, 'pattern_counts': {'":': 0, '<': 0, '<?xml version=': 0, '>': 0, 'https://': 0, 'lorem ipsum': 0, 'www.': 0, 'xml': 0}, 'pii_count': 0, 'substrings_counts': 0, 'word_list_counts': {'cursed_substrings.json': 0, 'profanity_word_list.json': 0, 'sexual_word_list.json': 0, 'zh_pornsignals.json': 0}}
Influence of a BGaN back-barrier on DC and dynamic performances of an AlGaN/GaN HEMT: simulation study

In this paper, we study the effect of a BGaN back-barrier on the DC and RF performances of an AlGaN/GaN high electron mobility transistor. Using TCAD Silvaco, we examine some variations of thickness and boron concentration in the BGaN back-barrier layer. First, we fix the thickness of the back-barrier layer at 5 nm and we vary the concentration of the boron in BGaN from 1% to 4%. Second, we fix the concentration of the boron in BGaN to only 2% and we vary the thickness of the back-barrier layer from 20 nm to 110 nm. The BGaN back-barrier layer creates an electrostatic barrier under the channel layer and improves the performances of the device by improving the electron confinement in the two-dimensional electron gas. The DC and AC characteristics are improved, respectively, by a greater concentration of boron and by a thicker BGaN layer. For 4% boron concentration and 5 nm thick back-barrier layer, we obtain a maximum drain current of 1.1 A, a maximum transconductance of 480 mS mm−1, a cut-off frequency of 119 GHz, and a maximum oscillation frequency of 311 GHz.