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After the Long Shutdown 2 the LHC will provide lead-lead collisions at interaction rates as high as 50kz. In order to cope with such conditions the ALICE Time Projection Chamber (TPC) needs to be upgraded. After the upgrade the TPC will run…

Instrumentation and Detectors · Physics 2019-08-12 Alexander Deisting

CONCERTO is a millimeter-wave imaging instrument that operated on the Atacama Pathfinder Experiment (APEX) telescope from April 2021 to May 2023. Its primary scientific objectives include the study of galaxy clusters through the…

Signal Processing · Electrical Eng. & Systems 2026-04-29 Mounir Abdkrimi , Olivier Rossetto , O. Bourrion , Christophe Vescovi , C. Hoarau

Thin pad detectors made from 75 $\mu$m thick epitaxial silicon on low resistivity substrate were irradiated with reactor neutrons to fluences from 2.5$\times 10^{16}$ n/cm$^2$ to 1$\times 10^{17}$ n/cm$^2$. Edge-TCT measurements showed that…

Instrumentation and Detectors · Physics 2020-12-30 I. Mandić , V. Cindro , A. Gorišek , B. Hiti , G. Kramberger , M. Mikuž , M. Zavrtanik , P. Skomina , S. Hidalgo , G. Pellegrini

We report the measurement of longitudinal electron diffusion coefficients in liquid argon for electric fields between 100 and 2000 V/cm with a gold photocathode as a bright electron source. The measurement principle, apparatus, and data…

Flexible Electronics (FE) offer distinct advantages, including mechanical flexibility and low process temperatures, enabling extremely low-cost production. To address the demands of applications such as smart sensors and wearables, flexible…

Hardware Architecture · Computer Science 2024-12-10 Paula Carolina Lozano Duarte , Florentia Afentaki , Georgios Zervakis , Mehdi B. Tahoori

For the upgrade of the inner tracker of the BESIII spectrometer, planned for 2018, a lightweight tracker based on an innovative Cylindrical Gas Electron Multiplier (CGEM) detector is now under development. The analogue readout of the CGEM…

An upgrade of the near detector of the T2K long baseline neutrino oscillation experiment is currently being conducted. This upgrade will include two new Time Projection Chambers, each equipped with 16 charge readout resistive Micromegas…

The PADME experiment, at the Laboratori Nazionali di Frascati (LNF), in Italy, will search for invisible decays of the hypothetical dark photon via the process $e^+e^-\rightarrow \gamma A'$, where the $A'$ escapes detection. The dark photon…

LHAASO project is to be built in south-west China, which use an array of 5137 election detectors for the measurement of the incident electrons arriving at the detector plane. For the quality control of the big quantity of electron…

Instrumentation and Detectors · Physics 2016-11-25 Xu Tongye , Du Yanyan , Shao Ruobin , Wang Xu , Zhu Chengguang

The beam parameters of complete prototype of the bERLinPro injector that consisted of a lead cathode in an 1.6 cell superconducting cavity were measured. The measurements are discussed in chapter 2 and indicate that the beam emittance is…

Accelerator Physics · Physics 2018-09-06 Martin Anton Helmut Schmeißer

This paper will discuss a new method of signal read-out from photon detectors in ultra-large, underground liquid argon time projection chambers. In this design, the signal from the light collection system is coupled via capacitive plates to…

Instrumentation and Detectors · Physics 2016-04-13 Z. Moss , M. Toups , L. Bugel , G. H. Collin , J. M. Conrad

Time-resolved electron microscopy aims at tracking nanoscale excitations and dynamic states of matter with a temporal resolution ultimately reaching the attosecond regime. Periodically time-varying fields in an illuminated specimen cause…

Dual-phase liquid xenon time projection chambers are the core detector elements of many experiments that conduct searches for Dark Matter and rare events, as well as in neutrino and high-energy physics. As part of this detector technology,…

The Short-Baseline Near Detector time projection chamber is unique in the design of its charge readout planes. These anode plane assemblies (APAs) have been fabricated and assembled to meet strict accuracy and precision requirements: wire…

Instrumentation and Detectors · Physics 2020-08-26 R. Acciarri , C. Adams , C. Andreopoulos , J. Asaadi , M. Babicz , C. Backhouse , W. Badgett , L. F. Bagby , D. Barker , C. Barnes , A. Basharina-Freshville , V. Basque , A. Baxter , M. C. Q. Bazetto , O. Beltramello , M. Betancourt , A. Bhanderi , A. Bhat , M. R. M. Bishai , A. Bitadze , A. S. T. Blake , J. Boissevain , C. Bonifazi , J. Y. Book , D. Brailsford , A. Brandt , J. Bremer , T. Brooks , B. A. Bullard , L. Camilleri , M. F. Carneiro , R. Castillo Fernández , M. Chalifour , Y. Chen , H. Chen , G. Chisnall , D. Cianci , J. I. Crespo-Anadón , E. Cristaldo , C. Cuesta , I. L. de Icaza Astiz , A. De Roeck , G. De Sá Pereira , G. de Souza , S. R. Dennis , L. Di Giulio , S. Dixon , A. Elvin , A. Ereditato , J. J. Evans , A. C. Ezeribe , C. Fabre , J. Farrell , R. S. Fitzpatrick , B. T. Fleming , N. Foppiani , W. Foreman , D. Franco , J. Freestone , A. P. Furmanski , T. Gamble , S. Gao , D. Garcia-Gamez , M. P. Garman , H. F. Gatti , G. Ge , I. Gil-Botella , S. Gollapinni , O. Goodwin , P. Green , W. C. Griffith , R. Guenette , P. Guzowski , P. Hamilton , S. Hentschel , C. M. Hill , A. Holin , S. Holt , J. Hrivnak , E. C. Huang , C. C. James , R. S. Jones , Y. Jwa , G. Karagiorgi , E. Kemp , M. J. Kim , U. Kose , I. Kreslo , S. Kubecki , V. A. Kudryavtsev , B. Lacarelle , M. R. Langstaff , J. Larkin , R. LaZur , I. Lepetic , B. R. Littlejohn , D. Lorca , W. C. Louis , A. A. Machado , M. Malek , C. Mariani , F. Marinho , A. Mastbaum , K. Mavrokoridis , N. McConkey , V. Meddage , I. Mercer , T. Mettler , K. Miller , K. Mistry , D. Mladenov , A. J. Mogan , J. Molina , M. Mooney , J. Mousseau , M. Nessi , S. Ni , R. Northrop , J. Nowak , O. Palamara , S. Palestini , C. Palomares , V. Pandey , J. R. Pater , L. Paulucci , Z. Pavlovic , D. Payne , O. L. G. Peres , O. Peres , F. Piastra , F. Pietropaolo , V. L. Pimentel , X. Pons , G. Putnam , X. Qian , V. Radeka , E. Raguzin , P. Ratoff , H. Ray , B. Rebel , M. Reggiani-Guzzo , F. Resnati , K. Rielage , A. Rigamonti , D. Rivera , M. Roda , M. Ross-Lonergan , G. Scanavini , A. Scarff , D. W. Schmitz , A. Schukraft , E. Segreto , E. Seletskaya , M. H. Shaevitz , J. Sinclair , R. Soares , M. Soderberg , S. Söldner-Rembold , H. V. Souza , F. Spagliardi , M. Spanu , J. Spitz , N. J. C. Spooner , M. Stancari , J. Statter , G. V. Stenico , T. Strauss , P. Sutcliffe , K. Sutton , A. M. Szelc , W. Tang , J. Tena Vidal , C. Thorn , R. T. Thornton , D. Torretta , M. Toups , C. Touramanis , M. Tripathi , S. Tufanli , E. Tyley , G. A. Valdiviesso , R. Van de Water , M. Weber , P. Wilson , A. Wilson , M. Worcester , E. Worcester , M. H. Wright , N. Wright , B. Yu , J. Yu , B. Zamorano , A. Zani , J. Zennamo , M. Zhao

Differentiating between an exoplanet signal and residual speckle noise is a key challenge in high-contrast imaging. Speckles are due to a combination of fast, slow and static wavefront aberrations introduced by atmospheric turbulence and…

For the high luminosity upgrade of the LHC at CERN, ATLAS is considering the addition of a High Granularity Timing Detector (HGTD) in front of the end cap and forward calorimeters at |z| = 3.5 m and covering the region 2.4 < |{\eta}| < 4 to…

The operation of Ultrafast Electron Diffractometers (UEDs) and Free-Electron Lasers (FELs) relies on high-brightness electron beams produced by radio-frequency (RF) photocathode guns. The next generation of high-repetition rate UEDs and…

Accelerator Physics · Physics 2021-05-18 Anatoliy Opanasenko , Zoltán Tibai , Kévin Pepitone , Georgii Shamuilov , Vitaliy Goryashko

Battery safety is paramount for electric vehicles. Early fault diagnosis remains a challenge due to the subtle nature of anomalies and the interference of dynamic operating noise. Existing data-driven methods often suffer from "physical…

Systems and Control · Electrical Eng. & Systems 2025-12-09 Jiong Yang

Operating HADES at the future FAIR SIS-100 accelerator challenges the rate capability of DAQ and electronics. A new, more robust version of front-end electronics needs to be built for the HADES drift chamber system. Due to the…

Instrumentation and Detectors · Physics 2018-11-19 Michael Wiebusch , Christian Müntz , Christian Wendisch , Jerzy Pietraszko , Jan Michel , Joachim Stroth

The Low-Energy Demonstration Accelerator (LEDA) radio-frequency quadrupole (RFQ) is a 100% duty factor (CW) linac that delivers >100 mA of H+ beam at 6.7 MeV. The 8-m-long, 350-MHz RFQ structure accelerates a dc, 75-keV, 110-mA H+ beam from…

Accelerator Physics · Physics 2012-08-27 M. E. Schulze , J. D. Gilpatrick , W. P. Lysenko , L. J. Rybarcyk , J. D. Schneider , H. V. Smith, , L. M. You