Lucian Fasselt , Ignacio Asensi Tortajada , Prafulla Behera , Dumitru Vlad Berlea , Daniela Bortoletto , Craig Buttar , Valerio Dao , Ganapati Dash , Leyre Flores Sanz de Acedo , Martin Gazi , Laura Gonella , Vicente González , Sebastian Haberl , Tomohiro Inada , Pranati Jana , Long Li , Heinz Pernegger , Petra Riedler , Walter Snoeys , Carlos Solans Sánchez , Steven Worm
{"title":"辐射硬耗尽单片有源像素传感器MALTA2的电荷校准","authors":"Lucian Fasselt , Ignacio Asensi Tortajada , Prafulla Behera , Dumitru Vlad Berlea , Daniela Bortoletto , Craig Buttar , Valerio Dao , Ganapati Dash , Leyre Flores Sanz de Acedo , Martin Gazi , Laura Gonella , Vicente González , Sebastian Haberl , Tomohiro Inada , Pranati Jana , Long Li , Heinz Pernegger , Petra Riedler , Walter Snoeys , Carlos Solans Sánchez , Steven Worm","doi":"10.1016/j.nima.2025.170972","DOIUrl":null,"url":null,"abstract":"<div><div>MALTA2 is a depleted monolithic active pixel sensor (DMAPS) designed for tracking at high rates and typically low detection threshold of <span><math><mrow><mn>200</mn><mspace></mspace><msup><mrow><mi>e</mi></mrow><mrow><mo>−</mo></mrow></msup></mrow></math></span>. Threshold calibration is crucial to understanding the charge collection in the pixel. A simple procedure is developed to calibrate the threshold to unit electrons making use of a dedicated charge injection circuit and an Fe-55 source with dominant charge deposition of <span><math><mrow><mn>1611</mn><mspace></mspace><msup><mrow><mi>e</mi></mrow><mrow><mo>−</mo></mrow></msup></mrow></math></span>. The injection voltage corresponding to the signal under exposure of Fe-55 is determined and serves as the basis for charge calibration. The charge injection circuit incorporates a capacitance with design value of <span><math><mrow><msub><mrow><mi>C</mi></mrow><mrow><mi>inj</mi></mrow></msub><mo>=</mo><mn>230</mn><mspace></mspace><mstyle><mi>a</mi><mi>F</mi></mstyle></mrow></math></span>. Experimentally, the average capacitance value for non-irradiated samples is found to be <span><math><mrow><msub><mrow><mi>C</mi></mrow><mrow><mi>inj,exp</mi></mrow></msub><mo>=</mo><mn>255</mn><mo>±</mo><mn>35</mn><mspace></mspace><mstyle><mi>a</mi><mi>F</mi></mstyle></mrow></math></span> and varies between sensors by 14% in terms of standard deviation. The deviation from the design value as well as among sensors motivates the need for the presented calibration procedure, which is proposed to be performed for each MALTA2 sensor and reduces the uncertainty down to 3% depending on the sensor.</div></div>","PeriodicalId":19359,"journal":{"name":"Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment","volume":"1082 ","pages":"Article 170972"},"PeriodicalIF":1.4000,"publicationDate":"2025-09-11","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Charge calibration of MALTA2, a radiation hard depleted monolithic active pixel sensor\",\"authors\":\"Lucian Fasselt , Ignacio Asensi Tortajada , Prafulla Behera , Dumitru Vlad Berlea , Daniela Bortoletto , Craig Buttar , Valerio Dao , Ganapati Dash , Leyre Flores Sanz de Acedo , Martin Gazi , Laura Gonella , Vicente González , Sebastian Haberl , Tomohiro Inada , Pranati Jana , Long Li , Heinz Pernegger , Petra Riedler , Walter Snoeys , Carlos Solans Sánchez , Steven Worm\",\"doi\":\"10.1016/j.nima.2025.170972\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><div>MALTA2 is a depleted monolithic active pixel sensor (DMAPS) designed for tracking at high rates and typically low detection threshold of <span><math><mrow><mn>200</mn><mspace></mspace><msup><mrow><mi>e</mi></mrow><mrow><mo>−</mo></mrow></msup></mrow></math></span>. Threshold calibration is crucial to understanding the charge collection in the pixel. A simple procedure is developed to calibrate the threshold to unit electrons making use of a dedicated charge injection circuit and an Fe-55 source with dominant charge deposition of <span><math><mrow><mn>1611</mn><mspace></mspace><msup><mrow><mi>e</mi></mrow><mrow><mo>−</mo></mrow></msup></mrow></math></span>. The injection voltage corresponding to the signal under exposure of Fe-55 is determined and serves as the basis for charge calibration. The charge injection circuit incorporates a capacitance with design value of <span><math><mrow><msub><mrow><mi>C</mi></mrow><mrow><mi>inj</mi></mrow></msub><mo>=</mo><mn>230</mn><mspace></mspace><mstyle><mi>a</mi><mi>F</mi></mstyle></mrow></math></span>. Experimentally, the average capacitance value for non-irradiated samples is found to be <span><math><mrow><msub><mrow><mi>C</mi></mrow><mrow><mi>inj,exp</mi></mrow></msub><mo>=</mo><mn>255</mn><mo>±</mo><mn>35</mn><mspace></mspace><mstyle><mi>a</mi><mi>F</mi></mstyle></mrow></math></span> and varies between sensors by 14% in terms of standard deviation. The deviation from the design value as well as among sensors motivates the need for the presented calibration procedure, which is proposed to be performed for each MALTA2 sensor and reduces the uncertainty down to 3% depending on the sensor.</div></div>\",\"PeriodicalId\":19359,\"journal\":{\"name\":\"Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment\",\"volume\":\"1082 \",\"pages\":\"Article 170972\"},\"PeriodicalIF\":1.4000,\"publicationDate\":\"2025-09-11\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S0168900225007740\",\"RegionNum\":3,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q3\",\"JCRName\":\"INSTRUMENTS & INSTRUMENTATION\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment","FirstCategoryId":"101","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0168900225007740","RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"INSTRUMENTS & INSTRUMENTATION","Score":null,"Total":0}
Charge calibration of MALTA2, a radiation hard depleted monolithic active pixel sensor
MALTA2 is a depleted monolithic active pixel sensor (DMAPS) designed for tracking at high rates and typically low detection threshold of . Threshold calibration is crucial to understanding the charge collection in the pixel. A simple procedure is developed to calibrate the threshold to unit electrons making use of a dedicated charge injection circuit and an Fe-55 source with dominant charge deposition of . The injection voltage corresponding to the signal under exposure of Fe-55 is determined and serves as the basis for charge calibration. The charge injection circuit incorporates a capacitance with design value of . Experimentally, the average capacitance value for non-irradiated samples is found to be and varies between sensors by 14% in terms of standard deviation. The deviation from the design value as well as among sensors motivates the need for the presented calibration procedure, which is proposed to be performed for each MALTA2 sensor and reduces the uncertainty down to 3% depending on the sensor.
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.