Dark current in multilayer stabilized amorphous selenium based photoconductive x-ray detectors

2012 ◽  
Vol 112 (1) ◽  
pp. 014502 ◽  
Author(s):  
Joel B. Frey ◽  
George Belev ◽  
Olivier Tousignant ◽  
Habib Mani ◽  
Luc Laperriere ◽  
...  
2009 ◽  
Vol 6 (S1) ◽  
pp. S251-S254 ◽  
Author(s):  
J. B. Frey ◽  
G. Belev ◽  
O. Tousignant ◽  
H. Mani ◽  
S. O. Kasap

2014 ◽  
Vol 92 (7/8) ◽  
pp. 641-644 ◽  
Author(s):  
M.Z. Kabir ◽  
Safayat-Al Imam

The density of defect states near the valence band of the hole blocking layer (commonly called the n-layer) is determined by analyzing the transient dark current behavior of multilayer amorphous selenium (a-Se) X-ray image detectors. The previous transient dark current model (Mahmood et al. Appl. Phys. Lett. 92, 223506 (2008)) is modified and compared with recently published experimental transient dark currents on commercial n-i-p and cold deposited n-i a-Se detector structures to determine the energy distributed deep defect densities in these two types of n-layer. The peak defect state exists at 0.75 and 0.78 eV from the valence band mobility edge in alkaline doped and cold deposited n-layers, respectively. The peak trap density in these n-layers varies in the range of 5 × 1016 – 5 × 1017 cm−3eV−1. The energy depths of the trap centers should be ∼(0.75–0.8) eV from the valence band mobility edge for a requirement of less transient time to reach a plateau. The shallower trap levels are unable to retain sufficient trapped charge to reduce the dark current, and the deeper trap centers create longer transient times to reach a steady level of dark current.


2008 ◽  
Author(s):  
M. Z. Kabir ◽  
F. Manouchehri ◽  
S. A. Mahmood ◽  
V. K. Devabhaktuni ◽  
O. Tousignant ◽  
...  

2008 ◽  
Vol 92 (22) ◽  
pp. 223506 ◽  
Author(s):  
S. A. Mahmood ◽  
M. Z. Kabir ◽  
O. Tousignant ◽  
H. Mani ◽  
J. Greenspan ◽  
...  

2008 ◽  
Vol 1066 ◽  
Author(s):  
Kyung-Wook Shin ◽  
Mohammad R. Esmaeili-Rad ◽  
Andrei Sazonov ◽  
Arokia Nathan

ABSTRACTHydrogenated nanocrystalline silicon (nc-Si:H) has strong potential to replace the hydrogenated amorphous silicon (a-Si:H) in thin film transistors (TFTs) due to its compatibility with the current industrial a-Si:H processes, and its better threshold voltage stability [1]. In this paper, we present an experimental TFT array backplane for direct conversion X-ray detector, using inverted staggered bottom gate nc-Si:H TFT as switching element. The TFTs employed a nc-Si:H/a-Si:H bilayer as the channel layer and hydrogenated amorphous silicon nitride (a-SiNx) as the gate dielectric; both layers deposited by plasma enhanced chemical vapor deposition (PECVD) at 280°C. Each pixel consists of a switching TFT, a charge storage capacitor (Cpx), and a mushroom electrode which serves as the bottom contact for X-ray detector such as amorphous selenium photoconductor. The chemical composition of the a-SiNx was studied by Fourier transform infrared spectroscopy. Current-voltage measurements of the a-SiNx film demonstrate that a breakdown field of 4.3 MV/cm.. TFTs in the array exhibits a field effect mobility (μEF) of 0.15 cm2/V·s, a threshold voltage (VTh) of 5.71 V, and a subthreshold leakage current (Isub) of 10−10 A. The fabrication sequence and TFT characteristics will be discussed in details.


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