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nEXO is a proposed next-generation experiment searching for the neutrinoless double beta decay of $^{136}$Xe using a tonne-scale liquid xenon (LXe) time projection chamber (TPC). To image the ionization signals from events in the liquid…

Instrumentation and Detectors · Physics 2025-12-15 Z. Li , M. Yu , E. Angelico , A. Atencio , A. Gupta , P. Knauss , A. Pena-Perez , B. G. Lenardo , P. Acharya , A. Amy , A. Anker , I. J. Arnquist , J. Bane , V. Belov , T. Bhatta , A. Bolotnikov , J. Breslin , P. A. Breur , J. P. Brodsky , E. Brown , T. Brunner , B. Burnell , E. Caden , G. F. Cao , L. Q. Cao , D. Cesmecioglu , D. Chernyak , M. Chiu , R. Collister , M. Marquis , T. Daniels , L. Darroch , R. DeVoe , M. L. di Vacri , X. Defay , Y. Y. Ding , D. Doering , M. J. Dolinski , A. Dragone , B. Eckert , A. Emara , N. Fatemighomi , W. Fairbank , B. T. Foust , D. Gallacher , N. Gallice , A. Gaur , W. Gillis , F. Girard , A. Gorham , K. Gracequist , G. Gratta , C. A. Hardy , J. Hasi , S. Hedges , M. Heffner , E. Hein , H. Hernandez Herrera , J. D. Holt , A. Iverson , X. S. Jiang , A. Karelin , D. Keblbeck , C. Kenney , I. Kotov , A. Kuchenkov , K. S. Kumar , S. Lavoie , A. Larson , M. B. Latif , K. G. Leach , D. S. Leonard , G. Lessard , K. K. H. Leung , G. Li , X. Li , C. Licciardi , R. Lindsay , R. MacLellan , S. Majidi , C. Malbrunot , B. Markovic , J. Masbou , M. Medina-Peregrina , S. Mngonyama , B. Mong , D. C. Moore , K. Ni , I. Nitu , A. Nolan , S. C. Nowicki , J. C. Nzobadila Ondze , A. Odian , J. L. Orrell , G. S. Ortega , L. Pagani , H. Peltz Smalley , A. Piepke , A. Pocar , S. Prentice , V. Radeka , E. Raguzin , R. Rai , H. Rasiwala , D. Ray , B. Reese , S. Rescia , F. Retiere , G. Richardson , V. Riot , R. Ross , L. Rota , P. C. Rowson , R. Saldanha , S. Sangiorgio , S. Sekula , T. Shetty , L. Si , F. Spadoni , V. Stekhanov , X. L. Sun , S. Thibado , T. Totev , S. Triambak , R. H. M. Tsang , O. A. Tyuka , T. Vallivilayil John , E. van Bruggen , M. Vidal , S. Viel , M. Walent , H. Wang , Q. D. Wang , M. Watts , W. Wei , M. Wehrfritz , L. J. Wen , S. Wilde , X. M. Wu , H. Xu , H. B. Yang , L. Yang , O. Zeldovich , J. Zhao

The Electron-Ion Collider provides a groundbreaking opportunity to study heavy pentaquarks with unprecedented precision, leveraging its high collision energy and beam spin polarization capabilities. As a representative case, we analyze…

High Energy Physics - Phenomenology · Physics 2025-03-05 In Woo Park , Sungtae Cho , Yongsun Kim , Su Houng Lee

The accumulation of positive ions, produced by ionizing particles crossing Liquid Argon Time Projection Chambers (LAr-TPCs), may generate distortions of the electric drift field affecting the track reconstruction of the ionizing events.…

In a multi-electrode device, the motion of free charge carriers generated by ionizing radiation induces currents on all the electrodes surrounding the active region [1]. The amount of charge induced in each sensitive electrode is a function…

Materials Science · Physics 2014-03-14 Jacopo Forneris , David Jamieson , Gabriele Giacomini , Changyi Yang , Ettore Vittone

Time projection chambers drifting negative ions (NITPC) instead of electrons have several advantages. A NITPC can operate at very high reduced drift fields without diffusion runaway, and the readout digitization sampling rate requirement is…

Atomic Physics · Physics 2010-04-22 M. P. Dion , C. J. Martoff , M. Hosack

Time Projection Chambers (TPCs) with charge readout via micro pattern gaseous detectors can provide detailed measurements of charge density distributions. We here report on measurements of alpha particle tracks, using a TPC where the drift…

Instrumentation and Detectors · Physics 2015-12-09 P. M. Lewis , S. E. Vahsen , M. T. Hedges , I. Jaegle , I. S. Seong , T. N. Thorpe

The LPCTrap experiment uses an open Paul trap which was built to enable precision measurements in the beta decay of radioactive ions. The initial goal was the precise measurement of the beta-neutrino angular correlation coefficient in the…

We propose a method to simultaneously correct linear optics errors and linear coupling for storage rings using turn-by-turn (TbT) beam position monitor (BPM) data. The independent component analysis (ICA) method is used to isolate the…

Accelerator Physics · Physics 2016-06-22 Xi Yang , Xiaobiao Huang

In this study, we developed a new proton detector system called CATCH, which was designed for a scattering experiment involving a $\Sigma$ hyperon and a proton (J-PARC E40). CATCH is a cylindrical detector system covering an inner target…

Instrumentation and Detectors · Physics 2022-03-14 Y. Akazawa , N. Chiga , N. Fujioka , S. H. Hayakawa , R. Honda , M. Ikeda , K. Matsuda , K. Miwa , Y. Nakada , T. Nanamura , S. Ozawa , T. Shiozaki , H. Tamura , H. Umetsu

ALICE is the CERN LHC experiment optimised for the study of the strongly interacting matter produced in heavy-ion collisions and devoted to the characterisation of the quark-gluon plasma. To achieve the physics program for LHC Run 3, a…

Instrumentation and Detectors · Physics 2020-12-04 Domenico Colella

The Electron-ion collider in China (EicC) is a proposed future electron-ion collider designed to achieve a high luminosity, with a center-of-mass energy ranging from 15 to 20 GeV. Excellent particle identification (PID) with extensive…

Instrumentation and Detectors · Physics 2026-05-25 Xin Li , Yuxiang Zhao , Yutie Liang , Xu Sun

The IDEA detector concept for a future e$^{+}$e$^{-}$ collider adopts an ultra-low mass drift chamber as a central tracking system. The He-based ultra-low mass drift chamber is designed to provide efficient tracking, a high-precision…

Although the MeV gamma-ray band is a promising energy-band window in astrophysics, the current situation of MeV gamma-ray astronomy significantly lags behind those of the other energy bands in angular resolution and sensitivity. An…

During the LHC Long Shutdown 3 (2026-29) ALICE will replace its three innermost tracking layers by a new detector, the "ITS3". It will be based on newly developed, wafer-scale monolithic active pixel sensors, which are bent into truly…

Instrumentation and Detectors · Physics 2026-01-13 Jory Sonneveld

During the high-luminosity phase of the LHC (HL-LHC), planned to start around 2027, the accelerator is expected to deliver an instantaneous peak luminosity of up to $7.5\times10^{34}$ cm$^{-2}$s$^{-1}$. A total integrated luminosity of…

Instrumentation and Detectors · Physics 2020-06-17 The Tracker Group of the CMS Collaboration

N$\nu$DEx aims to search for the neutrinoless double beta decay in $^{82}$Se using a high pressure $^{82}$SeF$_6$ gas time projection chamber (TPC). This paper presents a simulation and analysis framework developed specifically for the…

Instrumentation and Detectors · Physics 2026-03-04 Tianyu Liang , Hulin Wang , Dongliang Zhang , Chaosong Gao , Xiangming Sun , Feng Liu , Jun Liu , Chengui Lu , Yichen Yang , Chengxin Zhao , Hao Qiu , Kai Chen

ALICE (A Large Ion Collider Experiment) is the CERN LHC experiment optimized for the study of the strongly interacting matter produced in heavy-ion collisions and devoted to the characterization of the Quark-Gluon Plasma. To achieve the…

Instrumentation and Detectors · Physics 2019-12-30 Domenico Colella

A fundamental limit to the application of Time Projection Chambers (TPCs) in high-rate experiments is the accumulation of slowly drifting ions in the active gas volume, which compromises the homogeneity of the drift field and hence the…

Instrumentation and Detectors · Physics 2012-09-05 F. V. Böhmer , M. Ball , S. Dørheim , C. Höppner , B. Ketzer , I. Konorov , S. Neubert , S. Paul , J. Rauch , M. Vandenbroucke

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