Abstract:Narrow bandgap (<0.5 eV) colloidal semiconductor nanocrystals (e.g. mercury chalcogenides) provide practical platforms for next generation short wave infrared, mid wave infrared and long wave infrared optoelectronic devices. Until now, most of the efforts in the field of infrared active nanocrystals have been taken on synthesizing nanocrystals, determining quantum states and building different geometries for optoelectronic devices. However, studies on interface trap states in the devices made from these narrow… Show more
“…Various 0D materials, such as CsPbBr 3 quantum dots, HgTe nanocrystals, and PbS quantum dots, were hybridized with low-dimensional metal oxides to modulate the surface/interface charge behavior and optimize the photodetector performance. Due to the intriguing interfacial charge transfer behavior, the mixed dimensional heterojunction has shown fascinating properties beyond the individual metal oxides. − The decoration of 0D materials also changes the condition of the exposed material surface, thereby influencing the interaction of the photocarriers with chemisorbed foreign atoms or molecules. , Nitrogen-doped graphene quantum dots (NGQDs), an attractive carbon material, have extraordinary optical and electrical characteristics due to their pronounced quantum confinement and edge effects. The electron-rich nitrogen atoms endow NQGDs with extensive delocalized electrons and high charge carrier density, making them more favorable for potential optoelectronic devices. − NGQDs have been reported to exhibit superior electron transfer/reservoir properties when incorporated into metal oxides, resulting in the high sensing performance of the hybrid structure. − Moreover, compared with 0D materials mentioned above, NGQDs have the advantages of low toxicity, high chemical stability, and low cost .…”
The
long-time decay process induced by the persistent photoconductivity
(PPC) in metal oxides-based photodetectors (PDs) impedes our demands
for high-speed photodetectors. 2D perovskite oxides, emerging candidates
for future high-performance PDs, also suffer from the PPC effect.
Here, by integrating 2D perovskite Sr2Nb3O10 (SNO) nanosheets and nitrogen-doped graphene quantum dots
(NGQDs), a unique nanoscale heterojunction is designed to modulate
surface/interface carrier transport for enhanced response speed. Notably,
the decay time is reduced from hundreds of seconds to a few seconds.
The 4%NGQDs-SNO PD exhibits excellent performance with a photocurrent
of 0.47 μA, a high on–off ratio of 2.2 × 104, and a fast pulse response speed (τ
decay = 67.3 ms), making it promising for UV imaging.
The trap-involved decay process plays a dominant role in determining
the decay time, resulting in the PPC effect in SNO PD, and the trap
states mainly originate from oxygen vacancies and chemisorbed oxygen
molecules. A significantly enhanced photoresponse speed in NGQDs-SNO
PDs can be ascribed to the modulated surface/interface trap states
and the efficient carrier pathway provided by the nanoscale heterojunction.
This work provides an effective way to enhance the response speed
in 2D perovskite oxides constrained by PPC via surface/interface engineering,
promoting their applications in optoelectronics.
“…Various 0D materials, such as CsPbBr 3 quantum dots, HgTe nanocrystals, and PbS quantum dots, were hybridized with low-dimensional metal oxides to modulate the surface/interface charge behavior and optimize the photodetector performance. Due to the intriguing interfacial charge transfer behavior, the mixed dimensional heterojunction has shown fascinating properties beyond the individual metal oxides. − The decoration of 0D materials also changes the condition of the exposed material surface, thereby influencing the interaction of the photocarriers with chemisorbed foreign atoms or molecules. , Nitrogen-doped graphene quantum dots (NGQDs), an attractive carbon material, have extraordinary optical and electrical characteristics due to their pronounced quantum confinement and edge effects. The electron-rich nitrogen atoms endow NQGDs with extensive delocalized electrons and high charge carrier density, making them more favorable for potential optoelectronic devices. − NGQDs have been reported to exhibit superior electron transfer/reservoir properties when incorporated into metal oxides, resulting in the high sensing performance of the hybrid structure. − Moreover, compared with 0D materials mentioned above, NGQDs have the advantages of low toxicity, high chemical stability, and low cost .…”
The
long-time decay process induced by the persistent photoconductivity
(PPC) in metal oxides-based photodetectors (PDs) impedes our demands
for high-speed photodetectors. 2D perovskite oxides, emerging candidates
for future high-performance PDs, also suffer from the PPC effect.
Here, by integrating 2D perovskite Sr2Nb3O10 (SNO) nanosheets and nitrogen-doped graphene quantum dots
(NGQDs), a unique nanoscale heterojunction is designed to modulate
surface/interface carrier transport for enhanced response speed. Notably,
the decay time is reduced from hundreds of seconds to a few seconds.
The 4%NGQDs-SNO PD exhibits excellent performance with a photocurrent
of 0.47 μA, a high on–off ratio of 2.2 × 104, and a fast pulse response speed (τ
decay = 67.3 ms), making it promising for UV imaging.
The trap-involved decay process plays a dominant role in determining
the decay time, resulting in the PPC effect in SNO PD, and the trap
states mainly originate from oxygen vacancies and chemisorbed oxygen
molecules. A significantly enhanced photoresponse speed in NGQDs-SNO
PDs can be ascribed to the modulated surface/interface trap states
and the efficient carrier pathway provided by the nanoscale heterojunction.
This work provides an effective way to enhance the response speed
in 2D perovskite oxides constrained by PPC via surface/interface engineering,
promoting their applications in optoelectronics.
“…This process could be repeated over multiple cycles to reach a thick enough and contiguous conductive QD film. 1,2-Ethanedithiol (EDT) is a firm favourite choice as a short bifunctional ligand to be adopted for the ligand substitution of a series of spin/cast deposited films of Hg chalcogenide QDs, 10,68,75,79,[87][88][89][90][91] and for the HgTe/CdSe core-shell nanoplatelet (NPL) thin films. 92 The process should be done in a dry N 2 gas environment in a glove-box as the dithiol crosslinked film is sensitive to air and moisture exposure.…”
The commercial infrared (IR) photodetectors based on epitaxial growth inorganic semiconductors, e.g. InGaAs and HgCdTe, suffer from the high fabrication cost, poor compatibility with silicon integrated circuits, rigid substrate and...
“…Kolkovsky et al also demonstrated deep-level defects in a GaN NR ensemble using the DLTS technique [7]. Recently, the DLTS technique has been used to identify the deep traps in photodetector (PD) devices [8]. The trap states in the semiconductor mid-gap region restrict the photogenerated electrons from reaching the conduction band, so the photocurrent generation is inhibited in the device.…”
Understanding the metal/semiconductor interface is very significant for real-time optoelectronic device applications. In particular, the presence of interface states and other defects is detrimental to photodetector applications. In this study, the electrical transport properties of a pristine gallium nitride (GaN) nanorod (NR)-based Schottky diode are demonstrated at different temperatures by current–voltage characteristics in the range of 200–360 K. An enhancement in the Schottky barrier height (0.65 eV for hydrogen-passivated GaN NRs compared to 0.56 eV for pristine ones) is noticed. The effect of deep traps residing within the forbidden gap of GaN NRs is investigated using deep-level transient spectroscopy. Two deep defects are found at E
C − 0.19 eV and E
C − 0.31 eV in pristine GaN NRs; the E
C − 0.31 eV defect peak is attributed to V
Ga or nitrogen interstitials. After hydrogenation the peak at E
C − 0.31 eV is suppressed and that at E
C − 0.19 eV remains unchanged. The hydrogenated GaN NRs show a high photoresponse, which is nearly 2.83 times higher than that of pristine GaN NRs. The hydrogenated GaN NRs exhibit a photoresponsivity of 4.7
×
10−3 A W−1 and detectivity of 1.24
×
1010 Jones under UV illumination of λ = 382 nm. The enhanced performance is attributed to the deep defect passivation by hydrogenation along with the surface-state-free interface between the GaN NRs and metal contacts. The experimental results demonstrate the significance of hydrogen treatment use in the fabrication of GaN-based optoelectronic devices.
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