碲化镉β射线探测器

Morio Wada, Jun-Ichi Suzuki, Yuzo Ozaki
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引用次数: 9

摘要

介绍了一种用于β射线测厚仪的CdTe(碲化镉)探测器样机的制作和特点。探测器由一个pn结二极管组成,在没有外加电压的情况下以光伏模式工作。在0.01 V、30℃条件下,其暗电流小于7 × 10−14 A/mm2,无需制冷。在直径为16mm的有源区域上,在85Kr辐射条件下,输出电流为5 × 10−8 A,统计噪声为1.5 × 10−12 A/(Hz)12。探测器使用的(111)CdTe晶片尺寸为22 mm × 22 mm × 1.5 mm,采用无孪晶和低位错密度(小于1 × 106 cm−2)的单晶,因为发现与晶体缺陷(如孪晶和位错)有关的载流子的生成-重组中心会增加暗电流并降低输出电流。由于85Kr辐射源输出电流的温度系数约为0.23%/°C,因此采用热统计控制模块使探测器的工作温度恒定在0.1°C以内,从而解决了输出电流随温度漂移的问题。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Cadmium telluride β-ray detector

The fabrication and characteristics of a prototype CdTe (cadmium telluride) detector for a β-ray thickness gauge are described. The detector consists of a pn-junction diode, operating in photovoltaic mode with no applied voltage. It needs no cooling because its dark current is less than 7 × 10−14 A/mm2at 0.01 V and 30 °C. An output current of 5 × 10−8 A with a statistical noise of 1.5 × 10−12 A/(Hz)12 has been achieved with 85Kr radiation on an active area 16 mm in diameter. The (111) CdTe wafer used in the detector is 22 mm × 22 mm × 1.5 mm.

Single crystals with no twins and a low dislocation density (less than 1 × 106 cm−2) are used because it is found that the generation-recombination centres of carriers related to crystallographic defects (such as twins and dislocations) increase the dark current and decrease the output current.

As the temperature coefficient of the output current for an 85Kr radiation source is approximately 0.23%/°C, a thermostatistically-controlled module is used to keep the detector's operating temperature constant to within 0.1 °C, thus solving the problem of drift of output current with temperature.

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