Andrew Gentry, Maurizio Boscardin, Martin Hoeferkamp, Marco Povoli, Sally Seidel, Jiahe Si, Gian-Franco Dalla Betta
{"title":"25 \\mathrm{μm}$ 薄间距三维硅传感器中电荷倍增的证据\\25 \\mathrm{μm}$ 间距三维硅传感器中的电荷乘积","authors":"Andrew Gentry, Maurizio Boscardin, Martin Hoeferkamp, Marco Povoli, Sally Seidel, Jiahe Si, Gian-Franco Dalla Betta","doi":"arxiv-2409.03909","DOIUrl":null,"url":null,"abstract":"Characterization measurements of $25 \\mathrm{\\mu m} \\times 25 \\mathrm{\\mu m}$\npitch 3D silicon sensors are presented, for devices with active thickness of\n$150\\mu$m. Evidence of charge multiplication caused by impact ionization below\nthe breakdown voltage is observed. Small-pitch 3D silicon sensors have\npotential as high precision 4D tracking detectors that are also able to\nwithstand radiation fluences beyond $\\mathrm{10^{16} n_{eq}/cm^2}$, for use at\nfuture facilities such as the High-Luminosity Large Hadron Collider, the\nElectron-Ion Collider, and the Future Circular Collider. Characteristics of\nthese devices are compared to those for similar sensors of pitch $50\n\\mathrm{\\mu m} \\times 50 \\mathrm{\\mu m}$, showing comparable charge collection\nat low voltage, and acceptable leakage current, depletion voltage, breakdown\nvoltage, and capacitance despite the extremely small cell size. The\nunirradiated $25 \\mathrm{\\mu m} \\times 25 \\mathrm{\\mu m}$ sensors exhibit\ncharge multiplication above about 90 V reverse bias, while, as predicted, no\nmultiplication is observed in the $50 \\mathrm{\\mu m} \\times 50 \\mathrm{\\mu m}$\nsensors below their breakdown voltage. The maximum gain observed below\nbreakdown is 1.33.","PeriodicalId":501374,"journal":{"name":"arXiv - PHYS - Instrumentation and Detectors","volume":"5 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Evidence of Charge Multiplication in Thin $25 \\\\mathrm{μm} \\\\times 25 \\\\mathrm{μm}$ Pitch 3D Silicon Sensors\",\"authors\":\"Andrew Gentry, Maurizio Boscardin, Martin Hoeferkamp, Marco Povoli, Sally Seidel, Jiahe Si, Gian-Franco Dalla Betta\",\"doi\":\"arxiv-2409.03909\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Characterization measurements of $25 \\\\mathrm{\\\\mu m} \\\\times 25 \\\\mathrm{\\\\mu m}$\\npitch 3D silicon sensors are presented, for devices with active thickness of\\n$150\\\\mu$m. Evidence of charge multiplication caused by impact ionization below\\nthe breakdown voltage is observed. Small-pitch 3D silicon sensors have\\npotential as high precision 4D tracking detectors that are also able to\\nwithstand radiation fluences beyond $\\\\mathrm{10^{16} n_{eq}/cm^2}$, for use at\\nfuture facilities such as the High-Luminosity Large Hadron Collider, the\\nElectron-Ion Collider, and the Future Circular Collider. Characteristics of\\nthese devices are compared to those for similar sensors of pitch $50\\n\\\\mathrm{\\\\mu m} \\\\times 50 \\\\mathrm{\\\\mu m}$, showing comparable charge collection\\nat low voltage, and acceptable leakage current, depletion voltage, breakdown\\nvoltage, and capacitance despite the extremely small cell size. The\\nunirradiated $25 \\\\mathrm{\\\\mu m} \\\\times 25 \\\\mathrm{\\\\mu m}$ sensors exhibit\\ncharge multiplication above about 90 V reverse bias, while, as predicted, no\\nmultiplication is observed in the $50 \\\\mathrm{\\\\mu m} \\\\times 50 \\\\mathrm{\\\\mu m}$\\nsensors below their breakdown voltage. The maximum gain observed below\\nbreakdown is 1.33.\",\"PeriodicalId\":501374,\"journal\":{\"name\":\"arXiv - PHYS - Instrumentation and Detectors\",\"volume\":\"5 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-09-05\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"arXiv - PHYS - Instrumentation and Detectors\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/arxiv-2409.03909\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Instrumentation and Detectors","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.03909","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Evidence of Charge Multiplication in Thin $25 \mathrm{μm} \times 25 \mathrm{μm}$ Pitch 3D Silicon Sensors
Characterization measurements of $25 \mathrm{\mu m} \times 25 \mathrm{\mu m}$
pitch 3D silicon sensors are presented, for devices with active thickness of
$150\mu$m. Evidence of charge multiplication caused by impact ionization below
the breakdown voltage is observed. Small-pitch 3D silicon sensors have
potential as high precision 4D tracking detectors that are also able to
withstand radiation fluences beyond $\mathrm{10^{16} n_{eq}/cm^2}$, for use at
future facilities such as the High-Luminosity Large Hadron Collider, the
Electron-Ion Collider, and the Future Circular Collider. Characteristics of
these devices are compared to those for similar sensors of pitch $50
\mathrm{\mu m} \times 50 \mathrm{\mu m}$, showing comparable charge collection
at low voltage, and acceptable leakage current, depletion voltage, breakdown
voltage, and capacitance despite the extremely small cell size. The
unirradiated $25 \mathrm{\mu m} \times 25 \mathrm{\mu m}$ sensors exhibit
charge multiplication above about 90 V reverse bias, while, as predicted, no
multiplication is observed in the $50 \mathrm{\mu m} \times 50 \mathrm{\mu m}$
sensors below their breakdown voltage. The maximum gain observed below
breakdown is 1.33.