采用美光半导体制造的50 μm厚硅低增益雪崩探测器,时间分辨率为30ps

IF 1.4 3区 物理与天体物理 Q3 INSTRUMENTS & INSTRUMENTATION
R. Moriya , R. Bates , M. Bullough , N. Cooke , A. Docheva , L. Lombigit , D. Maneuski , R. McFeely , N. Moffat , M. Williams
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引用次数: 0

摘要

低增益雪崩探测器(lgad)是硅传感器与植入p掺杂倍增层,旨在提供增益之间的5和20。最重要的是,可以专门设计lgad以提供出色的时间分辨率。为了实现生产4D跟踪探测器的目标,必须优化LGAD技术,以获得优异的空间和时间分辨率。有希望的变体,如iLGAD和AC-LGAD,正在开发中。该技术在满足未来粒子物理实验的四维跟踪要求方面具有广阔的应用前景。美光半导体公司(Micron Semiconductor Ltd.)已经制造出活性厚度为50μm的lgad。通过电流-电压特性和瞬态电流技术(TCT)测量了电性能,同时使用Sr-90源的最小电离粒子(MIPs)测量了时序分辨率,并与IMB-CNM制造的器件进行了比较,以供参考。利用Sr-90源产生的MIPs,在−30°C的温度下测量,制备的器件的增益为5-10,定时分辨率为26.5 ps。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
30 ps time resolution with 50 μm thick silicon Low Gain Avalanche Detectors fabricated by Micron Semiconductor Ltd
Low Gain Avalanche Detectors (LGADs) are silicon sensors with an implanted p-doped multiplication layer that is designed to provide a gain between five and twenty. Most importantly, LGADs can be specifically engineered to provide excellent temporal resolution. To achieve the goal of producing a 4D tracking detector, where both excellent spatial and temporal resolution are attained, LGAD technology must be optimised. Promising variations, such as the iLGAD and AC-LGAD, are being developed. The technology shows promising prospects of fulfilling the 4D tracking requirements of future particle physics experiments. Micron Semiconductor Ltd. has fabricated LGADs with an active thickness of 50μm. The electrical performance has been measured by means of current–voltage characteristics and Transient Current Technique (TCT), while Minimum Ionising Particles (MIPs) from a Sr-90 source were used to measure the timing resolution, and compared with devices fabricated at IMB-CNM for reference. The fabricated devices were measured to have a gain of 5–10, a timing resolution of 26.5 ps using MIPs produced by a Sr-90 source, measured at a temperature of 30°C.
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来源期刊
CiteScore
3.20
自引率
21.40%
发文量
787
审稿时长
1 months
期刊介绍: Section A of Nuclear Instruments and Methods in Physics Research publishes papers on design, manufacturing and performance of scientific instruments with an emphasis on large scale facilities. This includes the development of particle accelerators, ion sources, beam transport systems and target arrangements as well as the use of secondary phenomena such as synchrotron radiation and free electron lasers. It also includes all types of instrumentation for the detection and spectrometry of radiations from high energy processes and nuclear decays, as well as instrumentation for experiments at nuclear reactors. Specialized electronics for nuclear and other types of spectrometry as well as computerization of measurements and control systems in this area also find their place in the A section. Theoretical as well as experimental papers are accepted.
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