1998
DOI: 10.1016/s0038-1101(97)00264-5
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Reverse currents of Schottky gates of III–V MESFET/HEMTs: field emission and tunnel currents

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Cited by 14 publications
(5 citation statements)
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“…Additionally, the thermionic-field emission and tunnelling mechanisms manifest the increase of leakage currents, since the carriers, acquiring sufficient energy, became 'hot' to dominate over the scattering effects and the Schottky barrier also decreased at high temperatures to facilitate the current injection or tunnelling. Therefore, the breakdown voltage is observed to decrease with temperature above 400 K [12]. The proposed device has also demonstrated higher turn-on and breakdown characteristics up to 500 K, as compared to the previous reports [8,9].…”
Section: Resultssupporting
confidence: 54%
“…Additionally, the thermionic-field emission and tunnelling mechanisms manifest the increase of leakage currents, since the carriers, acquiring sufficient energy, became 'hot' to dominate over the scattering effects and the Schottky barrier also decreased at high temperatures to facilitate the current injection or tunnelling. Therefore, the breakdown voltage is observed to decrease with temperature above 400 K [12]. The proposed device has also demonstrated higher turn-on and breakdown characteristics up to 500 K, as compared to the previous reports [8,9].…”
Section: Resultssupporting
confidence: 54%
“…7 plots the electric field profile at the gate interface, as the peak electric field at the gate edges is responsible for OFF-state breakdown. For a given Schottky barrier height and temperature, the OFF-state breakdown is dominated by TL electrons at high electric fields (> 900 kV/cm) and thermionic emission for low fields (< 150 kV/cm) [24]- [26]. As the peak electric field at the gate-drain edge (gate interface) is normally around 900 kV/cm, it is therefore under the high probability of breakdown.…”
Section: Resultsmentioning
confidence: 99%
“…BV gd is found to have increased from 12 to 19 V when we increased L gn+ from 0.3 to 0.5 μm. It is reported that the reverse bias breakdown mechanism in a pHEMT is based on the gate leakage current caused by the following possible mechanisms: impact ionization, TFE and tunnelling [5][6][7][8][9][10][11]. Here, BV gd is a strong function of peak electric field at gate edge towards drain.…”
Section: Resultsmentioning
confidence: 99%
“…Most of the studies interpreted the Schottky breakdown mechanism by the thermionic field emission (TFE) [5,6], tunnelling [5,[7][8][9], or impact ionization [9][10][11], in which BV gd is a strong function of peak electric field at the gate edge towards drain. Hence, the tailoring of peak electric field 0268-1242/12/115013+07$33.00 at the gate edge to lower values has been shown to be essential to improve BV gd [12][13][14][15][16][17].…”
Section: Introductionmentioning
confidence: 99%