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Muon-Induced X-ray Emission (MIXE) is a non-destructive analytical technique that leverages negative muons to probe elemental and isotopic compositions by detecting characteristic muonic X-rays emitted during atomic cascades and gamma rays…

A parametric simulation tool for pixel sensors is presented. A realistic pixel response is simulated purely based on measurement input, without requiring detailed knowledge of the underlying manufacturing process. As such, it provides an…

High-resolution 3D tracking with sub-nanosecond timing is required for the detection of elementary particles, such as neutrinos. Conventional detectors, which utilize analog silicon photomultipliers, face challenges in balancing spatial…

Instrumentation and Detectors · Physics 2025-11-24 Kodai Kaneyasu , Till Dieminger , Matthew Franks , Davide Sgalaberna , Claudio Bruschini , Edoardo Charbon

A prototype of the CMOS pixel sensor named SUPIX-1 has been fabricated and tested in order to investigate the feasibility of a pixelated tracker for a proposed Higgs factory, namely, the Circular Electron-Positron Collider (CEPC). The…

Instrumentation and Detectors · Physics 2022-01-05 L. Li , L. Zhang , J. N. Dong , J. Liu , M. Wang

Cosmic ray muon has strong penetrating power and no ionizing radiation hazards, which makes it an ideal probe for detecting special nuclear materials. In this paper, a high spatial resolution muon tomography system based on Micromegas…

Instrumentation and Detectors · Physics 2022-02-16 Yu Wang , Zhiyong Zhang , Shubin Liu , Zhongtao Shen , Changqing Feng , Jianguo Liu , Yulin Liu

The Super Tau-Charm Facility (STCF) is a proposed $e^+e^-$ collider with a peak luminosity 100 times higher than that of the present tau-charm factory. The inner tracker (ITK) of STCF should feature a low material budget and high readout…

The ATLAS experiment will undergo a major upgrade of the tracker system in view of the high luminosity phase of the LHC (HL-LHC) foreseen to start around 2025. Thin planar pixel modules are promising candidates to instrument the new pixel…

Instrumentation and Detectors · Physics 2017-03-08 N. Savic , L. Bergbreiter , J. Breuer , A. La Rosa , A. Macchiolo , R. Nisius , S. Terzo

The new Inner Tracking System (ITS2) is instrumental for tracking and vertex reconstruction in the ALICE experiment. The new tracker consists of seven cylindrical layers equipped with silicon Monolithic Active Pixel Sensors (MAPS) with a…

Instrumentation and Detectors · Physics 2025-05-21 A. Isakov

Monolithic Active Pixel Sensors (MAPS) have been developed since the late 1990s based on silicon substrates with a thin epitaxial layer (thickness of 10-15 $\mu$m) in which charge is collected on an electrode, albeit by disordered and slow…

We developed a beam telescope system comprising five layers of 300-$\mu$m-thick INTPIX4NA monolithic pixel sensors with each pixel size of 17 $\mu$m square. The sensors were fabricated using silicon-on-insulator (SOI) technology. The…

Instrumentation and Detectors · Physics 2022-08-24 Hisanori Suzuki , Takumi Omori , Kazuhiko Hara , Hiroki Yamauchi , Miho Yamada , Toru Tsuboyama , Ayaki Takeda

The ATLAS experiment will undergo a major upgrade of the tracker system in view of the high luminosity phase of the LHC (HL-LHC) to start operation in 2026. The most severe challenges are to be faced by the innermost layers of the pixel…

Instrumentation and Detectors · Physics 2016-12-06 Julien-Christopher Beyer , Alessandro La Rosa , Anna Macchiolo , Richard Nisius , Natascha Savic

The SUPerconduction AXion search experiment (Supax) is a haloscope designed to probe axion-like particles (ALPs) as candidates for dark matter and solutions to the strong CP problem. ALPs are predicted to couple to photons, allowing their…

High Energy Physics - Experiment · Physics 2025-05-13 Dhruv Chouhan , Tim Schneemann , Kristof Schmieden , Matthias Schott

To detect tracks of charged particles close to the interaction point in high energy physics experiments of the next generation colliders, hybrid pixel detectors, in which sensor and read-out IC are separate entities, constitute the present…

Instrumentation and Detectors · Physics 2010-01-22 N. Wermes

Pixel detectors for precise particle tracking in high energy physics have been developed to a level of maturity during the past decade. Three of the LHC detectors will use vertex detectors close to the interaction point based on the hybrid…

Instrumentation and Detectors · Physics 2007-05-23 Norbert Wermes

The MALTA CMOS monolithic silicon pixel sensors has been developed in the Tower 180 nm CMOS imaging process. It includes an asynchronous readout scheme and complies with the ATLAS inner tracker requirements for the HL-LHC. Several 4-chip…

We present an overview of the 'ICE' hardware and software framework that implements large arrays of interconnected FPGA-based data acquisition, signal processing and networking nodes economically. The system was conceived for application to…

Characterization of a hybrid ${\it telescope}$ with gas transmission detector ($\Delta$E) and a solid-state stop detector (E) has been fabricated for detection of low energy $\alpha$ particles between 5 to 1 MeV. The detector is developed…

Instrumentation and Detectors · Physics 2021-08-26 Rajkumar Santra , Subinit Roy

A novel approach for designing the next generation of vertex detectors foresees to employ wafer-scale sensors that can be bent to truly cylindrical geometries after thinning them to thicknesses of 20-40$\mu$m. To solidify this concept, the…

Instrumentation and Detectors · Physics 2021-08-18 ALICE ITS project , : , G. Aglieri Rinella , M. Agnello , B. Alessandro , F. Agnese , R. S. Akram , J. Alme , E. Anderssen , D. Andreou , F. Antinori , N. Apadula , P. Atkinson , R. Baccomi , A. Badalà , A. Balbino , C. Bartels , R. Barthel , F. Baruffaldi , I. Belikov , S. Beole , P. Becht , A. Bhatti , M. Bhopal , N. Bianchi , M. B. Blidaru , G. Boca , J. Bok , G. Bonomi , M. Bonora , M. Borri , V. Borshchov , E. Botta , G. E. Bruno , M. Buckland , S. Bufalino , M. Cai , P. Camerini , P. Cariola , F. Catalano , C. Ceballos Sanchez , I. Chakaberia , M. Chartier , F. Colamaria , D. Colella , A. Collu , M. Concas , G. Contin , S. Costanza , P. Cui , A. Dainese , J. B. Dainton , L. De Cilladi , C. De Martin , G. De Robertis , W. Deng , A. Di Mauro , Y. Ding , M. Durkac , D. Elia , M. R. Ersdal , M. Faggin , F. Fan , A. Fantoni , P. Fecchio , A. Feliciello , G. Feofilov , A. Ferk , J. Ferencei , G. Fiorenza , A. N. Flores , E. Fragiacomo , D. Gajanana , A. Gal , C. Gao , C. Gargiulo , P. Gianotti , P. Giubilato , A. Grant , L. Greiner , A. Grelli , O. S. Groettvik , F. Grosa , C. Guo Hu , R. Hannigan , J. A. Hasenbichler , H. Helstrup , H. Hillemanns , C. Hills , P. Hindley , B. Hippolyte , B. Hofman , G. H. Hong , G. Huang , J. P. Iddon , H. Ilyas , M. A. Imhoff , A. Isakov , A. Jadlovska , S. Jadlovska , J. Jadlovsky , S. Jaelani , T. Johnson , A. Junique , P. Kalinak , A. Kalweit , M. Keil , Z. Khabanova , H. Khan , B. Kim , C. Kim , J. Kim , J. Kim , T. Kim , J. Klein , A. Kluge , C. Kobdaj , A. Kotliarov , I. Králik , F. Krizek , T. Kugathasan , C. Kuhn , P. G. Kuijer , S. Kushpil , M. J. Kweon , J. Y. Kwon , Y. Kwon , P. La Rocca , A. Lakrathok , R. Langoy , P. Larionov , E. Laudi , T. Lazareva , R. Lea , R. C. Lemmon , X. L. Li , J. Lien , B. Lim , S. H. Lim , S. Lindsay , A. Liu , J. Liu , J. Liu , M. Lunardon , G. Luparello , M. Lupi , M. Mager , A. Maire , Q. W. Malik , G. Mandaglio , V. Manzari , Y. Mao , G. V. Margagliotti , C. Markert , D. Marras , P. Martinengo , S. Masciocchi , M. Masera , A. Masoni , A. Mastroserio , P. F. T. Matuoka , G. Mazza , F. Mazzaschi , M. A. Mazzoni , F Morel , V. Muccifora , A. Mulliri , L. Musa , S. V. Nesbo , D. Nesterov , J. Norman , J. Park , R. N Patra , C. Pastore , H. Pei , X. Peng , S. Piano , C. Pinto , S. Pisano , S. Politano , E. Prakasa , F. Prino , M. Protsenko , M. Puccio , A. Rachevski , L. Ramello , F. Rami , I. Ravasenga , A. Rehman , F. Reidt , F. Riggi , K. Røed , D. Röhrich , F. Ronchetti , A. Rosano , M. J. Rossewij , A. Rossi , R. Rui , R. Russo , R. Sadikin , V. Sarritzu , J. Schambach , S. Senyukov , J. J. Seo , R. Shahoyan , S. Shaukat , S. Siddhanta , M. Sitta , R. J. M. Snellings , W. Snoeys , A. Songmoolnak , J. Sonneveld , F. Soramel , M. Suljic , S. Sumowidagdo , D. Sun , X. Sun , G. J. Tambave , G. Tersimonov , M. Tkacik , M. Toppi , A. Trifiró , S. Trogolo , V. Trubnikov , R. Turrisi , T. S. Tveter , I. Tymchuck , K. Ullaland , M. Urioni , G. L. Usai , N. Valle , L. V. R. van Doremalen , T. Vanat , J. W. Van Hoorne , M. Varga-Kofarago , A. Velure , D. Wang , Y. Wang , J. Wikne , J. R. Wright , R. Xu , P. Yang , Z. Yin , I. -K. Yoo , J. H. Yoon , S. Yuan , V. Zaccolo , E. Zhang , X. Zhang , V. Zherebchevskii , D. Zhou , J. Zhu , Y. Zhu , G. Zinovjev , N. Zurlo

The Pixel Detector is the innermost detector of the tracking system of the Compact Muon Solenoid (CMS) experiment at CERN Large Hadron Collider (LHC). It precisely determines the interaction point (primary vertex) of the events and the…

Instrumentation and Detectors · Physics 2015-10-14 Chang-Seong Moon , Aurore Savoy-Navarro

We developed a novel design of a Micro Pixel Chamber ($\mu$-PIC) with resistive electrodes for a charged-particle-tracking detector in high-rate applications. Diamond-Like Carbon (DLC) thin film is used for the cathodes. The resistivity can…

Instrumentation and Detectors · Physics 2020-01-08 Fumiya Yamane , Atsuhiko Ochi , Kohei Matayoshi , Keisuke Ogawa , Yusuke Ishitobi