2011
DOI: 10.7567/jjap.50.04dg19
|View full text |Cite
|
Sign up to set email alerts
|

GaN-Based Metal–Semiconductor–Metal Ultraviolet Photodetectors with the ZrO2Insulating Layer

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
2

Citation Types

0
4
0

Year Published

2013
2013
2020
2020

Publication Types

Select...
7

Relationship

0
7

Authors

Journals

citations
Cited by 10 publications
(4 citation statements)
references
References 27 publications
0
4
0
Order By: Relevance
“…These limitations cause Schottky barrier inhomogeneity, , allow tunneling of carriers during reverse-bias conditions (in the dark), ,, and trap or recombine the photogenerated carriers. , In addition to this, lowering of Schottky barrier height, due to surface electronic states on GaN, is also responsible for allowing high reverse-bias current to flow in dark conditions, , thereby degrading the performance of the UV detector. Research has sought to alleviate these adverse effects by insertion of various oxide layers, such as Ta 2 O 5 , SiO 2 , ZrO 2 , Ga 2 O 3 , and HfO 2 , at the MS interface. These metal–insulator–semiconductor UV PDs have shown reduced dark current, which is beneficial to some extent. But there are a few constrains.…”
Section: Introductionmentioning
confidence: 99%
“…These limitations cause Schottky barrier inhomogeneity, , allow tunneling of carriers during reverse-bias conditions (in the dark), ,, and trap or recombine the photogenerated carriers. , In addition to this, lowering of Schottky barrier height, due to surface electronic states on GaN, is also responsible for allowing high reverse-bias current to flow in dark conditions, , thereby degrading the performance of the UV detector. Research has sought to alleviate these adverse effects by insertion of various oxide layers, such as Ta 2 O 5 , SiO 2 , ZrO 2 , Ga 2 O 3 , and HfO 2 , at the MS interface. These metal–insulator–semiconductor UV PDs have shown reduced dark current, which is beneficial to some extent. But there are a few constrains.…”
Section: Introductionmentioning
confidence: 99%
“…For example, Lee et al used a 130 nm thick GaO x interlayer for achieving a photo‐to‐dark current ratio of ≈10 6 where a peak responsivity of 9 A W −1 was demonstrated. On the other hand, Chen et al reported a photo‐to‐dark current ratio of ≈10 3 using only a 30 nm thick insulating layer of ZrO 2 where a peak responsivity of only 0.02 A W −1 was reported. Yet, in another report, a photo‐to‐dark current ratio of ≈10 4 and a peak responsivity of 1.42 A W −1 were demonstrated by inserting a very thin (only 1.5 nm) layer of HfO 2 .…”
Section: A Summary Of Schottky Junction Parameters Estimated Using Thmentioning
confidence: 79%
“…Insertion of an insulating layer between metal and semiconductor is an effective technique for suppressing the leakage current and also for improving an overall performance of PDs. A significant reduction in the leakage current is already reported by several researchers by incorporating various insulating layers, such as SiO 2 , ZrO 2 , GaO x , and Al 2 O 3 . Although a considerable amount of work is already carried out on GaN‐based metal–insulator–semiconductor (MIS) PDs, a consensus among researchers is yet to arrive on the choice of material and thickness of the insulating layer.…”
Section: A Summary Of Schottky Junction Parameters Estimated Using Thmentioning
confidence: 99%
“…Typical structures of photodetectors include p-n junction [13], p-i-n photodiode [14], i-n structure [15], Schottky barrier (SB) [16], metal-oxide-semiconductor (MOS) [17], metal-semiconductor-metal (MSM) [18,19], and photoelectrochemical cell (PEC) [20] based structures [21,22]. Among various UV photodetectors made of 1D nanostructures, PECbased photodetectors show promising potential due to their low cost, simple fabrication process and fast response.…”
Section: Introductionmentioning
confidence: 99%