2023
DOI: 10.1109/ted.2023.3258920
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Polarization Assisted Interdigital AlGaN/GaN Heterostructure Ultraviolet Photodetectors

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Cited by 12 publications
(4 citation statements)
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“…It can be calculated by the noise equivalent power (NEP): , D * = A × B NEP , where A is the active area, B is the electrical bandwidth. Generally, the NEP of the device can be estimated according to the equation: ,,, NEP = 2 q I D R , where q is the electronic charge constant and I D is the dark current density, and then the specific detectivity D * was calculated to be 4.36 × 10 16 Jones at 2 V. However, this specific detectivity value was overestimated because it only considered the short noise, but the noise of PDs commonly includes shot noise, thermal noise, and flicker (1/ f ) noise. , In order to more precisely measure specific detectivity, it is crucial to take into account the contribution of flicker noise at low frequency. Figure a shows the noise power spectra of PD measured in the frequency range of 1 to 100 kHz at various drain voltages.…”
Section: Resultsmentioning
confidence: 99%
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“…It can be calculated by the noise equivalent power (NEP): , D * = A × B NEP , where A is the active area, B is the electrical bandwidth. Generally, the NEP of the device can be estimated according to the equation: ,,, NEP = 2 q I D R , where q is the electronic charge constant and I D is the dark current density, and then the specific detectivity D * was calculated to be 4.36 × 10 16 Jones at 2 V. However, this specific detectivity value was overestimated because it only considered the short noise, but the noise of PDs commonly includes shot noise, thermal noise, and flicker (1/ f ) noise. , In order to more precisely measure specific detectivity, it is crucial to take into account the contribution of flicker noise at low frequency. Figure a shows the noise power spectra of PD measured in the frequency range of 1 to 100 kHz at various drain voltages.…”
Section: Resultsmentioning
confidence: 99%
“…Due to the strong polarization effects, high-concentration and high-mobility two-dimensional electron gases (2DEGs) often exist at the AlGaN/GaN heterojunction interface, which is quite beneficial to collect the photocurrent for high responsivity. Recently, several studies of PDs based on AlGaN/GaN 2DEGs have been reported. However, the 2DEG channel is naturally normally on even in the dark condition, which leads to high power consumption, low phototo-dark current ratio (PDCR) and poor detectivity. Several methods have been proposed to suppress the dark current for PDs, such as p-GaN gate, , semitransparent gate contact, p-oxide transparent gate, gate recessed .…”
Section: Introductionmentioning
confidence: 99%
“…The N-type ohmic contact layer consists of an N-type Al 0.1 Ga 0.9 N material with a high electron concentration. The layer is doped with a concentration of 1.0×10 18 cm -3 and has a thickness of 500 nm [10]. It is positioned on top of the buffer layer.…”
Section: Detector Structurementioning
confidence: 99%
“…8) The electric field profile can be homogenized by using such as the gated-edge termination, [9][10][11] tri-anode configuration, 12) field plates (FPs), [13][14][15][16][17][18] floating metal rings, 19,20) p-GaN termination [21][22][23][24] and polarization-induced electric field effect. 25) Among these candidates, FP structures have been widely used because of the easier technical process and the effective charge-coupling effect. The charge-coupling effect enables less Schottky barrier lowering effect, and then the leakage current can be decreased.…”
Section: Introductionmentioning
confidence: 99%