Detailed imager evaluation and unique applications of a new 20x25-cm size mercuric iodide thick film x-ray detector

Author(s):  
George Zentai ◽  
Larry D. Partain ◽  
Raisa Pavlyuchkova ◽  
Cesar Proano ◽  
Gary F. Virshup ◽  
...  
Keyword(s):  
2002 ◽  
Author(s):  
George Zentai ◽  
Larry D. Partain ◽  
Raisa Pavlyuchkova ◽  
Cesar Proano ◽  
Gary F. Virshup ◽  
...  

2006 ◽  
Author(s):  
Kyung-Jin Kim ◽  
Sang-Sik Kang ◽  
Ji-Koon Park ◽  
Sung-Ho Cho ◽  
Byung-Youl Cha ◽  
...  

2001 ◽  
Author(s):  
Michael M. Schieber ◽  
Haim Hermon ◽  
Asaf Zuck ◽  
Alexander I. Vilensky ◽  
Leonid Melekhov ◽  
...  

2016 ◽  
Vol 931 ◽  
pp. 47-56 ◽  
Author(s):  
Libu Manjakkal ◽  
Katarina Cvejin ◽  
Jan Kulawik ◽  
Krzysztof Zaraska ◽  
Robert P. Socha ◽  
...  

1993 ◽  
Vol 302 ◽  
Author(s):  
R. B. James ◽  
X. J. Bao ◽  
T. E. Schlesinger ◽  
A. Y. Cheng ◽  
V. M. Gerrish

ABSTRACTThe processing steps associated with purification of source material, crystal growth, and attachment of electrical contacts can introduce defects into mercuric iodide (HgI2) that degrade the performance of detectors. We have employed low-temperature photoluminescence (PL) spectroscopy to study radiative recombination centers in the interfacial region between a thin semitransparent film of silver and mercuric iodide. The Ag film was found to introduce a new broad emission band centered at 5490 Å in the photoluminescence spectrum of HgI2. This PL feature can be used as a signature to identify the existence of Ag as a contaminant in HgI2 crystals and detectors. Experiments were also conducted on mercuric iodide surfaces that had been doped with silver, and the results showed that Ag is a rapid diffuser in bulk HgI2. Detectors with silver electrodes were also fabricated and tested using an americium-241 gamma-ray source. Large increases in the leakage currents were observed for the Ag-doped HgI2 devices, indicated that Ag impurities are electrically active in HgI2. These measurements show that silver is unacceptable as an electrode material for mercuric iodide x-ray and gamma-ray detector applications. In addition, they reveal that caution must be taken during handling of mercuric iodide source material, crystals, and detectors to avoid contact with silver, silver compounds, or with any material that contains silver as a contaminant.


2020 ◽  
Author(s):  
Yongcheng Lu ◽  
Yuanxun Li ◽  
Daming Chen ◽  
Rui Peng ◽  
Qinghui Yang ◽  
...  

Abstract In order to explore an economical functional phase alternative material for thick film resistors, the crystal structure, microstructure, and electrical properties of (1-x)LSCN + xLCNZ (x = 0.0–1.0) composite ceramics were studied through solid-state reaction experiments. The composite ceramics were characterized by x–ray diffraction, scanning electron microscopy, energy dispersive x–ray spectroscopy, and DC four–probe method. Results suggested that the main phases of LSCN and LCNZ were formed, along with a small part of impurity phases. The addition of LCNZ to LSCN decreased the electrical conductivity and changed the TCR from positive to negative. Zero TCR could be achieved around 0.6 < x < 0.8 and relatively low absolute TCR values could be obtained for the samples of 0.4 ≤ x ≤ 0.8. The ceramic of 0.6LSCN + 0.4LCNZ showed the optimal performances of conductivity = 1923 S/cm, TCR = 379.54 ppm/℃, and relative density = 95.05%.


1980 ◽  
Vol 50 (3) ◽  
pp. 752-756 ◽  
Author(s):  
Samuel P. Faile ◽  
Andrzej J. Dabrowski ◽  
Gerald C. Huth ◽  
Jan S. Iwanczyk

1997 ◽  
Vol 493 ◽  
Author(s):  
D. Y. Noh ◽  
H. H. Lee ◽  
J. H. Je ◽  
H. K. Kim

ABSTRACTThe crystallization of amorphous BST thin films was studied in a synchrotron x-ray scattering experiment. At around 600°C, an intermediate phase, which was suspected to be a metastable pyrochlore phase, was formed. The x-ray reflectivity curves showed that the film-substrate interface became rough as the pyrochlore-like phase was formed. This suggests that the pyrochlore phase was nucleated near the interface area. Upon further annealing to higher temperatures, the film transformed to the crystalline perovskite phase. The crystallization was sensitive to the film thickness. In the thin 550Å thick film, the crystallization occurred at 750 °C with the <001> preferred orientation. On the other hand, the 5500Å thick film became crystalline even at 500°C with random crystalline orientation. The observed thickness dependence of the crystallization suggests that the crystalline perovskite phase was nucleated in the bulk of the film, rather than the near interface area.


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