Silicon detectors are the most widely used detector technology for precise tracking and vertex detectors at present experiments in particle physics. The requirements for future particle physics experiments are getting even more demanding, not only in required position resolution ( ∼ 𝑓 𝑒𝑤𝜇 m) and reduced pixel sizes, but also in ability to accurately, on the level of tens ps, measure the time of the particle hitting the detector. Among the hybrid pixel detectors there are two directions of developments. Thin Low gain avalanche detectors exploit internal gain to achieve required S/N and fast signal. On the other hand thicker 3D sensors exploit short drift distance given by vertical electrodes for fast charge collection and adequate signal. Monolithic Active Pixel Detectors offer a compromise between achievable signal/noise and thickness and recent developments exploiting also avalanche multiplication can offer excellent performance. The present paper will discuss basics, strengths and limitations of different technologies and possible directions of future developments.
{"title":"Silicon detectors for precision track timing","authors":"G. Kramberger","doi":"10.22323/1.420.0010","DOIUrl":"https://doi.org/10.22323/1.420.0010","url":null,"abstract":"Silicon detectors are the most widely used detector technology for precise tracking and vertex detectors at present experiments in particle physics. The requirements for future particle physics experiments are getting even more demanding, not only in required position resolution ( ∼ 𝑓 𝑒𝑤𝜇 m) and reduced pixel sizes, but also in ability to accurately, on the level of tens ps, measure the time of the particle hitting the detector. Among the hybrid pixel detectors there are two directions of developments. Thin Low gain avalanche detectors exploit internal gain to achieve required S/N and fast signal. On the other hand thicker 3D sensors exploit short drift distance given by vertical electrodes for fast charge collection and adequate signal. Monolithic Active Pixel Detectors offer a compromise between achievable signal/noise and thickness and recent developments exploiting also avalanche multiplication can offer excellent performance. The present paper will discuss basics, strengths and limitations of different technologies and possible directions of future developments.","PeriodicalId":275608,"journal":{"name":"Proceedings of 10th International Workshop on Semiconductor Pixel Detectors for Particles and Imaging — PoS(Pixel2022)","volume":"26 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2023-04-11","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"128834955","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Preface to the Proceedings of PIXEL2022","authors":"Sally Seidel","doi":"10.22323/1.420.0001","DOIUrl":"https://doi.org/10.22323/1.420.0001","url":null,"abstract":"","PeriodicalId":275608,"journal":{"name":"Proceedings of 10th International Workshop on Semiconductor Pixel Detectors for Particles and Imaging — PoS(Pixel2022)","volume":"35 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2023-03-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"129459419","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Hadron Damage Investigation of FBK and HPK Low Gain Avalanche Detectors","authors":"J. Sorenson","doi":"10.22323/1.420.0044","DOIUrl":"https://doi.org/10.22323/1.420.0044","url":null,"abstract":"","PeriodicalId":275608,"journal":{"name":"Proceedings of 10th International Workshop on Semiconductor Pixel Detectors for Particles and Imaging — PoS(Pixel2022)","volume":"21 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2023-03-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"134029636","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Yuma Aoki, Yamato Ito, M. Nobukawa, Y. Kanemaru, Keitaro Miyazaki, Kohei Kusunoki, K. Mori, T. Yoneyama, T. Tamba, H. Tomida, H. Nakajima, H. Matsumoto, H. Noda, K. Hayashida, H. Uchida, Takaaki Tanaka, Hiromasa Suzuki, Tessei Yoshida, H. Murakami, M. Yamauchi, I. Hatsukade, K. Hagino, T. Kohmura, H. Uchiyama, K. Yamaoka, M. Ozaki, T. Dotani, H. Tsunemi, K. Nobukawa, T. Tsuru, S. Kobayashi, J. Hiraga
We have developed a soft X-ray telescope system Xtend onboard Japan’s new X-ray astronomical satellite XRISM. Xtend employs X-ray CCDs, which have basically the same design as those used in the previous X-ray astronomical satellite Hitomi. Monochromatic X-ray line spectra of the CCDs onboard Hitomi showed offsets of centroids between different pixel patterns or different good grades; the spectral centroids of charge-sharing events are higher than those of single-pixel events. The spectral offset, which we call “Goffset”, can cause large uncertainties in X-ray energy determination accuracy. In this paper, confirming the CCDs onboard XRISM also have Goffset, we performed a simulation study that takes into account the two factors; charge sharing and readout noise. Goffset of the flight model CCD is successfully reproduced by the simulation with a certain readout noise. We investigate how charge sharing and readout noise cause Goffset based on the simulation results.
{"title":"Simulation Study of Pulse Height Difference Between Pixel Patterns of X-ray CCDs Onboard the XRISM Satellite","authors":"Yuma Aoki, Yamato Ito, M. Nobukawa, Y. Kanemaru, Keitaro Miyazaki, Kohei Kusunoki, K. Mori, T. Yoneyama, T. Tamba, H. Tomida, H. Nakajima, H. Matsumoto, H. Noda, K. Hayashida, H. Uchida, Takaaki Tanaka, Hiromasa Suzuki, Tessei Yoshida, H. Murakami, M. Yamauchi, I. Hatsukade, K. Hagino, T. Kohmura, H. Uchiyama, K. Yamaoka, M. Ozaki, T. Dotani, H. Tsunemi, K. Nobukawa, T. Tsuru, S. Kobayashi, J. Hiraga","doi":"10.22323/1.420.0036","DOIUrl":"https://doi.org/10.22323/1.420.0036","url":null,"abstract":"We have developed a soft X-ray telescope system Xtend onboard Japan’s new X-ray astronomical satellite XRISM. Xtend employs X-ray CCDs, which have basically the same design as those used in the previous X-ray astronomical satellite Hitomi. Monochromatic X-ray line spectra of the CCDs onboard Hitomi showed offsets of centroids between different pixel patterns or different good grades; the spectral centroids of charge-sharing events are higher than those of single-pixel events. The spectral offset, which we call “Goffset”, can cause large uncertainties in X-ray energy determination accuracy. In this paper, confirming the CCDs onboard XRISM also have Goffset, we performed a simulation study that takes into account the two factors; charge sharing and readout noise. Goffset of the flight model CCD is successfully reproduced by the simulation with a certain readout noise. We investigate how charge sharing and readout noise cause Goffset based on the simulation results.","PeriodicalId":275608,"journal":{"name":"Proceedings of 10th International Workshop on Semiconductor Pixel Detectors for Particles and Imaging — PoS(Pixel2022)","volume":"20 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2023-03-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"133845054","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Leticia Braga Da Rosa, Larissa Mendes, Renato Negrao de Oliveira, Guilherme Paulino, Sara Santos, Robert Tartarotti, Pedro Oliveira, Thiago Barbosa, Alessandra Tomal
The X-ray techniques used in synchrotron sources have been an indispensable tool in studying the physical aspects of various fields, such as biology, chemistry, and materials science. The results of these experiments often depend on the performance of the detectors, especially when studying sample dynamics, which require fast and sensitive X-ray detectors. This work presents a description of the PIMEGA X-ray camera system based on 1 mm thick CdTe sensors with a 55 μ m pixel pitch bump-bonded to Medipix3RX ASICs. It is also described the preliminary results of the system’s prototype characterization and imaging capabilities, which were conducted in terms of spatial resolution, detective quantum efficiency, leakage current, full depletion, and equalization responses. The experiments were performed using the detector in super high gain mode, with a 12-bit configuration in Fine Pitch and Single-Pixel mode. The results show the high-quality imaging capabilities of the detector with excellent values of MTF and DQE.
{"title":"Characterization of Hybrid Pixel Detector With CdTe Sensor","authors":"Leticia Braga Da Rosa, Larissa Mendes, Renato Negrao de Oliveira, Guilherme Paulino, Sara Santos, Robert Tartarotti, Pedro Oliveira, Thiago Barbosa, Alessandra Tomal","doi":"10.22323/1.420.0057","DOIUrl":"https://doi.org/10.22323/1.420.0057","url":null,"abstract":"The X-ray techniques used in synchrotron sources have been an indispensable tool in studying the physical aspects of various fields, such as biology, chemistry, and materials science. The results of these experiments often depend on the performance of the detectors, especially when studying sample dynamics, which require fast and sensitive X-ray detectors. This work presents a description of the PIMEGA X-ray camera system based on 1 mm thick CdTe sensors with a 55 μ m pixel pitch bump-bonded to Medipix3RX ASICs. It is also described the preliminary results of the system’s prototype characterization and imaging capabilities, which were conducted in terms of spatial resolution, detective quantum efficiency, leakage current, full depletion, and equalization responses. The experiments were performed using the detector in super high gain mode, with a 12-bit configuration in Fine Pitch and Single-Pixel mode. The results show the high-quality imaging capabilities of the detector with excellent values of MTF and DQE.","PeriodicalId":275608,"journal":{"name":"Proceedings of 10th International Workshop on Semiconductor Pixel Detectors for Particles and Imaging — PoS(Pixel2022)","volume":"72 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2023-03-13","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"114498372","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
M. Ressegotti, G. Calderini, F. Crescioli, G. Dalla Betta, G. Gariano, C. Gemme, F. Guescini, S. Hadzic, T. Heim, A. Lapertosa, S. Ravera, A. Rummler, M. Samy, L. Vannoli, D. Sultan
The ITk detector, the new ATLAS silicon tracking system for the High Luminosity LHC (HL-LHC), will be equipped with 3D pixel sensor modules in the innermost layer (L0). The pixel cell dimensions will be 25 × 100 µ m 2 in the barrel and 50 × 50 µ m 2 in the end-caps, with one readout electrode at the centre of each pixel and four bias electrodes at the corners. Sensors from pre-production wafers (50 × 50 µ m 2 ) produced by FBK have been bump-bonded to ITkPixV1.1 chips at IZM. Bare modules have been assembled in Genoa on Single Chip Cards (SCCs) and characterized in laboratory measurements and in test beam campaigns. Some of these modules have been irradiated in Bonn and at the CERN IRRAD facility. Preliminary results of their characterization after irradiation
ITk探测器是用于高亮度大型强子对撞机(HL-LHC)的新型ATLAS硅跟踪系统，将在最内层(L0)配备3D像素传感器模块。筒体的像素单元尺寸为25 × 100 μ m 2，端盖的像素单元尺寸为50 × 50 μ m 2，每个像素的中心有一个读出电极，角落有四个偏置电极。FBK生产的预生产晶圆(50 × 50 μ m 2)的传感器已与IZM的ITkPixV1.1芯片碰撞结合。裸模块已经在热那亚的单芯片卡(SCCs)上组装，并在实验室测量和测试光束运动中进行了表征。其中一些模组已在波恩和欧洲核子研究中心辐照研究中心设施照射过。辐照后表征的初步结果
{"title":"Qualification of the first pre-production 3D FBK sensors with ITkPixV1 readout chip","authors":"M. Ressegotti, G. Calderini, F. Crescioli, G. Dalla Betta, G. Gariano, C. Gemme, F. Guescini, S. Hadzic, T. Heim, A. Lapertosa, S. Ravera, A. Rummler, M. Samy, L. Vannoli, D. Sultan","doi":"10.22323/1.420.0025","DOIUrl":"https://doi.org/10.22323/1.420.0025","url":null,"abstract":"The ITk detector, the new ATLAS silicon tracking system for the High Luminosity LHC (HL-LHC), will be equipped with 3D pixel sensor modules in the innermost layer (L0). The pixel cell dimensions will be 25 × 100 µ m 2 in the barrel and 50 × 50 µ m 2 in the end-caps, with one readout electrode at the centre of each pixel and four bias electrodes at the corners. Sensors from pre-production wafers (50 × 50 µ m 2 ) produced by FBK have been bump-bonded to ITkPixV1.1 chips at IZM. Bare modules have been assembled in Genoa on Single Chip Cards (SCCs) and characterized in laboratory measurements and in test beam campaigns. Some of these modules have been irradiated in Bonn and at the CERN IRRAD facility. Preliminary results of their characterization after irradiation","PeriodicalId":275608,"journal":{"name":"Proceedings of 10th International Workshop on Semiconductor Pixel Detectors for Particles and Imaging — PoS(Pixel2022)","volume":"56 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2023-03-13","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"114580218","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
The increase of the particle flux (pile-up) at the HL-LHC with instantaneous luminosities up to 𝐿 ≃ 7 . 5 × 10 34 cm − 1 s − 2 will have a severe impact on the ATLAS detector reconstruction and trigger performance. The end-cap and forward region where the liquid Argon calorimeter has coarser granularity and the inner tracker has poorer momentum resolution will be particularly affected. A High Granularity Timing Detector (HGTD) will be installed in front of the LAr end-cap calorimeters for pile-up mitigation and luminosity measurement. The HGTD is a novel detector introduced to assist the new all-silicon Inner Tracker (ITk) in the pseudo-rapidity range from 2.4 to 4.0, adding the capability to measure charged-particle trajectories in time as well as space. Two silicon-sensor double-sided layers will provide precision timing information for minimum-ionising particles with a resolution as good as 30 ps per track to help disentangle tracks from different vertices in the same bunch crossing. Readout cells have a size of 1.3 mm × 1.3 mm, leading to a highly granular detector with 3.7 million channels. Low Gain Avalanche Detectors (LGAD) technology has been chosen as it provides enough gain to reach the large signal over noise ratio needed. The requirements and overall specifications of the HGTD will be presented as well as the technical design and the project status. The on-going R&D effort carried out to study the sensors, the readout ASIC, and the other components, supported by laboratory and test beam results, will also be presented.
{"title":"A High Granularity Timing Detector for the ATLAS Phase II Upgrade","authors":"Afonso Soares Canas Ferreira","doi":"10.22323/1.420.0013","DOIUrl":"https://doi.org/10.22323/1.420.0013","url":null,"abstract":"The increase of the particle flux (pile-up) at the HL-LHC with instantaneous luminosities up to 𝐿 ≃ 7 . 5 × 10 34 cm − 1 s − 2 will have a severe impact on the ATLAS detector reconstruction and trigger performance. The end-cap and forward region where the liquid Argon calorimeter has coarser granularity and the inner tracker has poorer momentum resolution will be particularly affected. A High Granularity Timing Detector (HGTD) will be installed in front of the LAr end-cap calorimeters for pile-up mitigation and luminosity measurement. The HGTD is a novel detector introduced to assist the new all-silicon Inner Tracker (ITk) in the pseudo-rapidity range from 2.4 to 4.0, adding the capability to measure charged-particle trajectories in time as well as space. Two silicon-sensor double-sided layers will provide precision timing information for minimum-ionising particles with a resolution as good as 30 ps per track to help disentangle tracks from different vertices in the same bunch crossing. Readout cells have a size of 1.3 mm × 1.3 mm, leading to a highly granular detector with 3.7 million channels. Low Gain Avalanche Detectors (LGAD) technology has been chosen as it provides enough gain to reach the large signal over noise ratio needed. The requirements and overall specifications of the HGTD will be presented as well as the technical design and the project status. The on-going R&D effort carried out to study the sensors, the readout ASIC, and the other components, supported by laboratory and test beam results, will also be presented.","PeriodicalId":275608,"journal":{"name":"Proceedings of 10th International Workshop on Semiconductor Pixel Detectors for Particles and Imaging — PoS(Pixel2022)","volume":"30 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2023-03-13","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"127884258","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
The inner tracking system (ITS2) of the ALICE experiment is foreseen to be upgraded during the Long Shutdown 3 of the Large Hadron Collider (LHC). First data are expected to be taken during Run 4 with the upgraded High-Luminosity LHC. The planned ITS3 detector will be based on stitched, wafer-scale Monolithic Active Pixel Sensors (MAPS), bent to radii of 18, 24, and 30 mm and fabricated on 300 mm wafers in a 65 nm CMOS Imaging technology. They will be thinned down to below 50 µ m and held in place by carbon foam spacers, resulting in an unprecedented material budget of O(0.05%) 𝑋 / 𝑋 0 per layer. This contribution will present the detector concept, summarise the results of the R&D program, including most recent 65 nm prototypes, and provide an outlook on the path towards the final sensor development.
{"title":"The ALICE Pixel Sensor Upgrade","authors":"L. Lautner","doi":"10.22323/1.420.0026","DOIUrl":"https://doi.org/10.22323/1.420.0026","url":null,"abstract":"The inner tracking system (ITS2) of the ALICE experiment is foreseen to be upgraded during the Long Shutdown 3 of the Large Hadron Collider (LHC). First data are expected to be taken during Run 4 with the upgraded High-Luminosity LHC. The planned ITS3 detector will be based on stitched, wafer-scale Monolithic Active Pixel Sensors (MAPS), bent to radii of 18, 24, and 30 mm and fabricated on 300 mm wafers in a 65 nm CMOS Imaging technology. They will be thinned down to below 50 µ m and held in place by carbon foam spacers, resulting in an unprecedented material budget of O(0.05%) 𝑋 / 𝑋 0 per layer. This contribution will present the detector concept, summarise the results of the R&D program, including most recent 65 nm prototypes, and provide an outlook on the path towards the final sensor development.","PeriodicalId":275608,"journal":{"name":"Proceedings of 10th International Workshop on Semiconductor Pixel Detectors for Particles and Imaging — PoS(Pixel2022)","volume":"24 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2023-03-13","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"117087530","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
During the long shutdown 4 of the LHC the instantaneous luminosity will be increased by a factor of ≈ 10 to 1 . 5 · 10 34 cm − 2 s − 1 . The expected data recorded with the LHCb detector will increase from 50 fb − 1 to 300 fb − 1 . This will require an upgrade of the LHCb tracking systems. For the downstream tracker this upgrade detector is referred to as the Mighty Tracker. The innermost part of the Mighty Tracker is planned to be instrumented with monolithic CMOS sensors. The outer part will keep the scintillating fibre approach of the currently installed SciFi detector. There are several aspects that make this a unique environment for a tracking detector. The high occupancy in the high 𝜂 region of LHCb (hit rates up to 18 MHz/cm 2 ), the harsh radiation conditions (6 · 10 14 1 MeV n eq / cm 2 ), the streaming readout approach with low material budget ( 𝑋 / 𝑋 0 < 1 . 5%) requirements are just naming a few key challenges. This can be achieved by newly developed HV-CMOS sensors which can provide a high timing resolution of ≈ 3 ns and are sufficiently radiation hard. The planned total instrumented pixel area is up to 18 m 2 of silicon. This paper will describe the plans for the Mighty Tracker and initial beam tests with the precursor of the MightyPix chip.
{"title":"The LHCb Mighty Tracker","authors":"K. Padeken","doi":"10.22323/1.420.0084","DOIUrl":"https://doi.org/10.22323/1.420.0084","url":null,"abstract":"During the long shutdown 4 of the LHC the instantaneous luminosity will be increased by a factor of ≈ 10 to 1 . 5 · 10 34 cm − 2 s − 1 . The expected data recorded with the LHCb detector will increase from 50 fb − 1 to 300 fb − 1 . This will require an upgrade of the LHCb tracking systems. For the downstream tracker this upgrade detector is referred to as the Mighty Tracker. The innermost part of the Mighty Tracker is planned to be instrumented with monolithic CMOS sensors. The outer part will keep the scintillating fibre approach of the currently installed SciFi detector. There are several aspects that make this a unique environment for a tracking detector. The high occupancy in the high 𝜂 region of LHCb (hit rates up to 18 MHz/cm 2 ), the harsh radiation conditions (6 · 10 14 1 MeV n eq / cm 2 ), the streaming readout approach with low material budget ( 𝑋 / 𝑋 0 < 1 . 5%) requirements are just naming a few key challenges. This can be achieved by newly developed HV-CMOS sensors which can provide a high timing resolution of ≈ 3 ns and are sufficiently radiation hard. The planned total instrumented pixel area is up to 18 m 2 of silicon. This paper will describe the plans for the Mighty Tracker and initial beam tests with the precursor of the MightyPix chip.","PeriodicalId":275608,"journal":{"name":"Proceedings of 10th International Workshop on Semiconductor Pixel Detectors for Particles and Imaging — PoS(Pixel2022)","volume":"28 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2023-03-13","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"123988290","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
The pixel tracking detectors in the ATLAS and CMS experiments are scheduled to be replaced with upgraded versions during the next long shutdown period at the LHC. The upgraded detectors are designed to take advantage of the high-luminosity operation of the LHC which is due to begin in 2029. This means that the active sensor area must increase
{"title":"Overview on Current State of the Art Pixel Mechanics for the Upgrade Tracking Detectors at the ATLAS and CMS Experiments","authors":"O. Shea","doi":"10.22323/1.420.0074","DOIUrl":"https://doi.org/10.22323/1.420.0074","url":null,"abstract":"The pixel tracking detectors in the ATLAS and CMS experiments are scheduled to be replaced with upgraded versions during the next long shutdown period at the LHC. The upgraded detectors are designed to take advantage of the high-luminosity operation of the LHC which is due to begin in 2029. This means that the active sensor area must increase","PeriodicalId":275608,"journal":{"name":"Proceedings of 10th International Workshop on Semiconductor Pixel Detectors for Particles and Imaging — PoS(Pixel2022)","volume":"11 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2023-03-13","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"127477836","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
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