论文标题
受α辐射的中子辐射的4H-silicon碳化物二极管的性能
Performance of neutron-irradiated 4H-Silicon Carbide diodes subjected to Alpha radiation
论文作者
论文摘要
4H-Silicon-Carbide(4H-SIC)的独特电和材料特性使其成为高速粒子探测器的有前途的候选材料。与普遍使用的硅(SI)相比,4H-SIC提供了更高的载体饱和速度和较大的击穿电压,从而实现了高内在的时间分辨率和缓解堆积效应。此外,随着辐射硬度需求的增加越来越苛刻,诸如4H-SIC之类的宽带材料可以提供更好的性能。在这项工作中,在室温下研究了50微米厚的4H-SIC P-in-N平面传感器的检测器性能,使用241am Alpha源在高达1100 V的反向偏差下进行的Alpha源。在研究中包括经过1E16/cm^2的中性辐照的样品,以量化辐射硬度性能,以量化1E16/CM^2的频率。将获得的结果与先前进行的UV-TCT研究进行了比较。样品表现出充电效率(CCE)的下降,随着辐照的增加,在高偏置电压下部分补偿了远高于全耗尽电压的高反向偏置电压。根据体积的耗竭,α颗粒穿透了未辐照的参考探测器,观察到收集的电荷的平台。对于中子辐照的样品,这种平稳性仅在较高的反向偏置下变得明显。对于最高研究的通量,CCE几乎与反向偏置的增加线性行为。与UV-TCT测量值相比,由于α颗粒的穿透深度较小,耗尽敏感体积覆盖全能量的敏感体积所需的反向偏置较低。在反向偏差最高的情况下,测得的CCE值与早期的UV-TCT研究非常吻合,差异在1%至5%之间。
The unique electrical and material properties of 4H-silicon-carbide (4H-SiC) make it a promising candidate material for high rate particle detectors. In contrast to the ubiquitously used silicon (Si), 4H-SiC offers a higher carrier saturation velocity and larger breakdown voltage, enabling a high intrinsic time resolution and mitigating pile-up effects. Additionally, as radiation hardness requirements grow more demanding, wide-bandgap materials such as 4H-SiC could offer better performance. In this work, the detector performance of 50 micron thick 4H-SiC p-in-n planar pad sensors was investigated at room temperature, using an 241Am alpha source at reverse biases of up to 1100 V. Samples subjected to neutron irradiation with fluences of up to 1e16/cm^2 were included in the study in order to quantify the radiation hardness properties of 4H-SiC. The obtained results are compared to previously performed UV-TCT studies. Samples exhibit a drop in charge collection efficiency (CCE) with increasing irradiation fluence, partially compensated at high reverse bias voltages far above full depletion voltage. A plateau of the collected charges is observed in accordance with the depletion of the volume the alpha particles penetrate for an unirradiated reference detector. For the neutron-irradiated samples, such a plateau only becomes apparent at higher reverse bias. For the highest investigated fluence, CCE behaves almost linearly with increasing reverse bias. Compared to UV-TCT measurements, the reverse bias required to deplete a sensitive volume covering full energy deposition is lower, due to the small penetration depth of the alpha particles. At the highest reverse bias, the measured CCE values agree well with earlier UV-TCT studies, with discrepancies between 1% and 5%.