1997
DOI: 10.1016/s0927-796x(96)00199-4
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Mercuric iodide for room temperature radiation detectors. Synthesis, purification, crystal growth and defect formation

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Cited by 37 publications
(18 citation statements)
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“…However, these materials have their own disadvantages such as poor hole charge transport properties and high cost for CZT single crystals, 7,30-33 phase transitions from red α-phase to yellow β-phase over ~127 o C for HgI 2 , 34 and polarization for TlBr. 35 Because of these issues, new superior detector grade materials are in demand.…”
Section: Introductionmentioning
confidence: 99%
“…However, these materials have their own disadvantages such as poor hole charge transport properties and high cost for CZT single crystals, 7,30-33 phase transitions from red α-phase to yellow β-phase over ~127 o C for HgI 2 , 34 and polarization for TlBr. 35 Because of these issues, new superior detector grade materials are in demand.…”
Section: Introductionmentioning
confidence: 99%
“…Most studies on α-HgI 2 , whether fundamental or as a potential ionizing radiation detector were performed on single crystals [9][10][11][12][13]. However, growing single crystals with homogeneous and reproducible detection performances turned to be a very difficult task [14][15][16][17][18].…”
Section: Introductionmentioning
confidence: 99%
“…Mercuric iodide (HgI 2 ) is one of the most suitable semiconductor materials for γ-ray and X-ray detectors operating at room temperature because of its favorable characteristics, such as high atomic number of its constituent elements and large band gap (2.13 eV), resulting in a high photopeak efficiency [1][2][3]. High-energy radiation detectors have high resolution ability to γ-ray and X-ray at room temperature, which were fabricated with HgI 2 [4][5][6][7].…”
Section: Introductionmentioning
confidence: 99%