{"title":"用于气体像素探测器的低噪声、低功耗像素传感器芯片","authors":"Zhuo Zhou, Shi-Qiang Zhou, Dong Wang, Xiang-Ming Sun, Chao-Song Gao, Peng-Zhen Zhu, Wei-Ping Ren, Jun Liu, Mu-Xian Li, Chen Lian, Chun-Lai Dong","doi":"10.1007/s41365-024-01418-0","DOIUrl":null,"url":null,"abstract":"<p>Topmetal-M2 is a large-area pixel sensor chip fabricated using the GSMC <span>\\(130\\,\\textrm{nm}\\)</span> CMOS process in 2021. The pixel array of Topmetal-M2 consists of pixels of 400 rows <span>\\(\\times\\)</span> 512 columns with a pixel pitch of <span>\\(45\\,\\mathrm {\\mu m} \\times 45\\,\\mathrm {\\mu m}\\)</span>. The array is divided into 16 subarrays, with pixels of 400 rows <span>\\(\\times\\)</span> 32 columns per subarray. Each pixel incorporates two charge sensors: a diode sensor and a Topmetal sensor. The in-pixel circuit primarily consists of a charge-sensitive amplifier for energy measurements, a discriminator with a peak-holding circuit, and a time-to-amplitude converter for time-of-arrival measurements. The pixel of Topmetal-M2 has a charge input range of <span>\\(\\sim 0{-}3\\,\\mathrm {k\\,e^-}\\)</span>, a voltage output range of <span>\\(\\sim 0{-}180\\,\\textrm{mV}\\)</span>, and a charge-voltage conversion gain of <span>\\(\\sim 59.56\\,\\mathrm {\\mu V/e^-}\\)</span>. The average equivalent noise charge of Topmetal-M2, which includes the readout electronic system noise, is <span>\\(\\sim 43.45\\,\\mathrm {e^-}\\)</span>. In the scanning mode, the time resolution of Topmetal-M2 is <span>\\(1\\,\\textrm{LSB} = 1.25\\,\\mathrm {\\mu s}\\)</span>, and the precision is <span>\\(\\sim 7.41\\,\\mathrm {\\mu s}\\)</span>. At an operating voltage of <span>\\(1.5\\,\\textrm{V}\\)</span>, Topmetal-M2 has a power consumption of <span>\\(\\sim 49\\,\\mathrm {mW/cm^2}\\)</span>. In this article, we provide a comprehensive overview of the chip architecture, pixel working principles, and functional behavior of Topmetal-M2. Furthermore, we present the results of preliminary tests conducted on Topmetal-M2, namely, alpha-particle and soft X-ray tests.</p>","PeriodicalId":19177,"journal":{"name":"Nuclear Science and Techniques","volume":"12 1","pages":""},"PeriodicalIF":3.6000,"publicationDate":"2024-05-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Low-noise and low-power pixel sensor chip for gas pixel detectors\",\"authors\":\"Zhuo Zhou, Shi-Qiang Zhou, Dong Wang, Xiang-Ming Sun, Chao-Song Gao, Peng-Zhen Zhu, Wei-Ping Ren, Jun Liu, Mu-Xian Li, Chen Lian, Chun-Lai Dong\",\"doi\":\"10.1007/s41365-024-01418-0\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p>Topmetal-M2 is a large-area pixel sensor chip fabricated using the GSMC <span>\\\\(130\\\\,\\\\textrm{nm}\\\\)</span> CMOS process in 2021. The pixel array of Topmetal-M2 consists of pixels of 400 rows <span>\\\\(\\\\times\\\\)</span> 512 columns with a pixel pitch of <span>\\\\(45\\\\,\\\\mathrm {\\\\mu m} \\\\times 45\\\\,\\\\mathrm {\\\\mu m}\\\\)</span>. The array is divided into 16 subarrays, with pixels of 400 rows <span>\\\\(\\\\times\\\\)</span> 32 columns per subarray. Each pixel incorporates two charge sensors: a diode sensor and a Topmetal sensor. The in-pixel circuit primarily consists of a charge-sensitive amplifier for energy measurements, a discriminator with a peak-holding circuit, and a time-to-amplitude converter for time-of-arrival measurements. The pixel of Topmetal-M2 has a charge input range of <span>\\\\(\\\\sim 0{-}3\\\\,\\\\mathrm {k\\\\,e^-}\\\\)</span>, a voltage output range of <span>\\\\(\\\\sim 0{-}180\\\\,\\\\textrm{mV}\\\\)</span>, and a charge-voltage conversion gain of <span>\\\\(\\\\sim 59.56\\\\,\\\\mathrm {\\\\mu V/e^-}\\\\)</span>. The average equivalent noise charge of Topmetal-M2, which includes the readout electronic system noise, is <span>\\\\(\\\\sim 43.45\\\\,\\\\mathrm {e^-}\\\\)</span>. In the scanning mode, the time resolution of Topmetal-M2 is <span>\\\\(1\\\\,\\\\textrm{LSB} = 1.25\\\\,\\\\mathrm {\\\\mu s}\\\\)</span>, and the precision is <span>\\\\(\\\\sim 7.41\\\\,\\\\mathrm {\\\\mu s}\\\\)</span>. At an operating voltage of <span>\\\\(1.5\\\\,\\\\textrm{V}\\\\)</span>, Topmetal-M2 has a power consumption of <span>\\\\(\\\\sim 49\\\\,\\\\mathrm {mW/cm^2}\\\\)</span>. In this article, we provide a comprehensive overview of the chip architecture, pixel working principles, and functional behavior of Topmetal-M2. Furthermore, we present the results of preliminary tests conducted on Topmetal-M2, namely, alpha-particle and soft X-ray tests.</p>\",\"PeriodicalId\":19177,\"journal\":{\"name\":\"Nuclear Science and Techniques\",\"volume\":\"12 1\",\"pages\":\"\"},\"PeriodicalIF\":3.6000,\"publicationDate\":\"2024-05-03\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Nuclear Science and Techniques\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://doi.org/10.1007/s41365-024-01418-0\",\"RegionNum\":1,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q1\",\"JCRName\":\"NUCLEAR SCIENCE & TECHNOLOGY\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Nuclear Science and Techniques","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1007/s41365-024-01418-0","RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"NUCLEAR SCIENCE & TECHNOLOGY","Score":null,"Total":0}
Low-noise and low-power pixel sensor chip for gas pixel detectors
Topmetal-M2 is a large-area pixel sensor chip fabricated using the GSMC \(130\,\textrm{nm}\) CMOS process in 2021. The pixel array of Topmetal-M2 consists of pixels of 400 rows \(\times\) 512 columns with a pixel pitch of \(45\,\mathrm {\mu m} \times 45\,\mathrm {\mu m}\). The array is divided into 16 subarrays, with pixels of 400 rows \(\times\) 32 columns per subarray. Each pixel incorporates two charge sensors: a diode sensor and a Topmetal sensor. The in-pixel circuit primarily consists of a charge-sensitive amplifier for energy measurements, a discriminator with a peak-holding circuit, and a time-to-amplitude converter for time-of-arrival measurements. The pixel of Topmetal-M2 has a charge input range of \(\sim 0{-}3\,\mathrm {k\,e^-}\), a voltage output range of \(\sim 0{-}180\,\textrm{mV}\), and a charge-voltage conversion gain of \(\sim 59.56\,\mathrm {\mu V/e^-}\). The average equivalent noise charge of Topmetal-M2, which includes the readout electronic system noise, is \(\sim 43.45\,\mathrm {e^-}\). In the scanning mode, the time resolution of Topmetal-M2 is \(1\,\textrm{LSB} = 1.25\,\mathrm {\mu s}\), and the precision is \(\sim 7.41\,\mathrm {\mu s}\). At an operating voltage of \(1.5\,\textrm{V}\), Topmetal-M2 has a power consumption of \(\sim 49\,\mathrm {mW/cm^2}\). In this article, we provide a comprehensive overview of the chip architecture, pixel working principles, and functional behavior of Topmetal-M2. Furthermore, we present the results of preliminary tests conducted on Topmetal-M2, namely, alpha-particle and soft X-ray tests.
期刊介绍:
Nuclear Science and Techniques (NST) reports scientific findings, technical advances and important results in the fields of nuclear science and techniques. The aim of this periodical is to stimulate cross-fertilization of knowledge among scientists and engineers working in the fields of nuclear research.
Scope covers the following subjects:
• Synchrotron radiation applications, beamline technology;
• Accelerator, ray technology and applications;
• Nuclear chemistry, radiochemistry, radiopharmaceuticals, nuclear medicine;
• Nuclear electronics and instrumentation;
• Nuclear physics and interdisciplinary research;
• Nuclear energy science and engineering.