2019
DOI: 10.1021/acsami.9b00940
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Self-Integrated Hybrid Ultraviolet Photodetectors Based on the Vertically Aligned InGaN Nanorod Array Assembly on Graphene

Abstract: Integration of one-dimensional (1D) semiconductors with two-dimensional (2D) materials into hybrid systems is identified as promising applications for new optoelectronic and photodetection devices. Herein, a selfintegrated hybrid ultraviolet (UV) photodetector based on InGaN nanorod arrays (NRAs) sandwiched between transparent top and back graphene contacts forming a Schottky junction has been demonstrated for the first time. The controlled van der Waals epitaxy of the vertically aligned InGaN NRA assembly on … Show more

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Cited by 48 publications
(43 citation statements)
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“…Furthermore, the corresponding photoresponsivity ( R λ ) and photodetectivity ( D* ) are generally two important factors to evaluate the photodetection performance of a photodetector device. The R λ can be obtained by the Equation (1) [ 44 ] Rλ = IphIdarkP S where I ph and I dark are the measured photocurrent under illumination and the dark current, respectively; P is the incident light power intensity; and S is the effective irradiated area (2500 µm 2 ) of photodetector. Moreover, the D* can be calculated by the following Equation (2) [ 33 ] D = Rλ A1/22eIdark1/2 where e is the electron charge; and A is the active area between channels of photodetector.…”
Section: Resultsmentioning
confidence: 99%
“…Furthermore, the corresponding photoresponsivity ( R λ ) and photodetectivity ( D* ) are generally two important factors to evaluate the photodetection performance of a photodetector device. The R λ can be obtained by the Equation (1) [ 44 ] Rλ = IphIdarkP S where I ph and I dark are the measured photocurrent under illumination and the dark current, respectively; P is the incident light power intensity; and S is the effective irradiated area (2500 µm 2 ) of photodetector. Moreover, the D* can be calculated by the following Equation (2) [ 33 ] D = Rλ A1/22eIdark1/2 where e is the electron charge; and A is the active area between channels of photodetector.…”
Section: Resultsmentioning
confidence: 99%
“…Moreover, suitable band edge position for water redox reaction, long charge diffuse distance, high surface‐to‐volume ratio and outstanding theoretical solar‐to‐hydrogen (STH) efficiency (≈27%) make InGaN nanorods highly beneficial for PEC overall water splitting. [ 10–12 ] However, the fatal drawbacks such as rapid bulk and surface charge recombination and sluggish oxidation reaction kinetic of InGaN nanorods result in an additional bias required to promote photoextracted charge transfer. [ 13,14 ] Nowadays, constructing semiconductors heterostructure to modulate the energy band of the heterojunction has been considered as one of the most effective methods to promote bulk and surface charge separation.…”
Section: Introductionmentioning
confidence: 99%
“…The epitaxy caused by a 2-D material, termed van der Waals epitaxy (vdWE), reduces the dislocation density of the grown material, which strongly affects the device properties, and also allows exfoliation of the grown material from the substrate owing to the weak chemical bond. [1][2][3][4] The advantages of vdWE have been conrmed using various structures, such as gallium nitride (GaN) or aluminium nitride (AlN) growth on graphene/silicon carbide (SiC), 5 graphene/ silicon dioxide (SiO 2 ), [6][7][8][9] graphene/silicon (Si), [10][11][12] graphene/ sapphire (Al 2 O 3 ), [13][14][15][16][17][18] and hexagonal boron nitride (h-BN)/ Al 2 O 3 . 19,20 However, the remaining dislocation density on vdWE is still a hurdle to achieving high-quality semiconductors.…”
Section: Introductionmentioning
confidence: 99%