基于cdte的X射线和γ射线探测器的空间电荷限制传输

O. Maslyanchuk, M. Solovan, V. Kulchynsky, V. Gnatyuk, T. Aoki
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引用次数: 1

摘要

限制CdTe和cdmnte基X/γ射线探测器光谱性能的主要特征是由于泄漏电流增大而无法提高工作电压以提供足够的载流子收集。我们对CdTe和cdmnte基双欧姆触点探测器的电特性进行了详细的分析。结果表明,在CdTe和CdMnTe晶体中施加高偏置电压时,泄漏电流的快速增加是由空间电荷(SCLC)限制的电流引起的。平衡空穴电流和非平衡空穴在高压下产生的电流具有相同的活化能,这证实了Ni/CdMnTe/Ni探测器中的SCLC是由于注入多数载流子(空穴)而在不完美欧姆触点处降低势垒而形成的。这一事实将Ni/CdMnTe/Ni探测器与Pt/CdTe/Pt探测器区别开,在Pt/CdTe/Pt探测器中,SCLC是由少数载流子通过晶体和金属接触面之间的薄绝缘膜从金属中的费米能级(或略低于它)到半导体的隧道跃迁形成的。根据Mott-Gurney理论,比较不同温度下CdMnTe晶体的测量值和计算值的电流-电压特性,可以确定Ni/CdMnTe/Ni探测器中离散俘获中心的密度(1.4 × 1013 cm3)和空穴阱的能量(0.39 eV)。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Space-charge limited transport in CdTe-based X- and γ-ray detectors
The principle feature limiting spectrometric performance of CdTe and CdMnTe-based X/γ-ray detectors is the impossibility to increase the operating voltage to provide sufficient collection of charge carriers because of raising leakage current. We have carried out the detailed analysis of electrical characteristics of CdTe and CdMnTe-based detectors with two Ohmic contacts. It is shown that a rapid increase in leakage current at applying high bias voltage in the CdTe and CdMnTe crystals is caused by the current limited by space charge (SCLC). The same activation energy for the current of equilibrium holes and the current caused by nonequilibrium holes at high voltages confirms the fact that SCLC in the Ni/CdMnTe/Ni detector formed by injection of majority carriers (holes) due to lowering the barrier at an imperfect Ohmic contacts. This fact distinguishes Ni/CdMnTe/Ni detector from Pt/CdTe/Pt detector where SCLC formed by tunnel transitions of minority carriers from the Fermi level in the metal (or slightly below it) to the semiconductor through a thin insulating film between the crystal and metal contact. Comparison the measured and calculated current-voltage characteristics of CdMnTe crystal at different temperatures taking into account SCLC according to the Mott-Gurney theory allowed to determine the density of discrete trapping centers (1.4 × 1013 cm3) and energy of hole traps (0.39 eV) in the Ni/CdMnTe/Ni detector.
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