Characterization results of MAPS digital prototypes for the ALICE ITS3

Anna Villani, the ALICE Collaboration
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引用次数: 0

Abstract

The three innermost layers of the ALICE Inner Tracking System (ITS2) will be replaced by a truly cylindrical tracker, the ITS3, to be ready for LHC Run 4 (2029–2032). The ITS3 will be composed of three layers, each made by two self-supporting, ultra-thin (50μm) flexible Monolithic Active Pixel silicon Sensors (MAPS) of large area (O(10 × 26 cm2)). The final sensor will be realized using the 65 nm CMOS imaging process and stitching technology. Multiple small-scale test structures were included in the first production run (Multiple Layer Reticle 1 - MLR1) to validate the 65 nm CMOS imaging technology. First large-scale stitched MAPS were included in the second production run (Engineering Run 1 - ER1). The pixel cell performance has been qualified on the MLR1 Digital Pixel Test Structures (DPTS) in laboratory and with in-beam measurements. The large-area (1.4 × 25.9 cm2) ER1 MOnolithic Stitched Sensor (MOSS) prototype has been used to prove the stitching principle and evaluate the detection efficiency and spatial resolution. This contribution will give an overview of the most recent results of the digital prototype tests.
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用于 ALICE ITS3 的 MAPS 数字原型的表征结果
ALICE 内部跟踪系统(ITS2)最里面的三层将被真正的圆柱形跟踪器 ITS3 取代,为大型强子对撞机运行 4(2029-2032 年)做好准备。ITS3 将由三层组成,每层由两个自支撑、超薄(≤50μm)、大面积(O(10 × 26 cm2))柔性单片有源像素硅传感器(MAPS)构成。最终的传感器将采用 65 纳米 CMOS 成像工艺和拼接技术来实现。在首次生产运行(多层视网膜 1 - MLR1)中包含了多个小规模测试结构,以验证 65 纳米 CMOS 成像技术。在第二次生产运行(工程运行 1 - ER1)中首次采用了大规模拼接 MAPS。像素单元的性能已在实验室的 MLR1 数字像素测试结构(DPTS)上得到验证,并进行了光束内测量。大面积(1.4 × 25.9 cm2)ER1 MOnolithic Stitched 传感器(MOSS)原型已用于验证拼接原理,并评估探测效率和空间分辨率。本文将概述数字原型测试的最新结果。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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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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