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We successfully carried out the first high-altitude balloon flight of a wide-field hard X-ray coded-aperture telescope ProtoEXIST1, which was launched from the Columbia Scientific Balloon Facility at Ft. Sumner, New Mexico on October 9,…

Instrumentation and Methods for Astrophysics · Physics 2015-05-28 J. Hong , B. Allen , J. Grindlay , S. Barthelemy , R. Baker , A. Garson , H. Krawczynski , J. Apple , W. H. Cleveland

CLIC is a proposed linear $e^+e^-$ collider with center-of-mass energies of up to 3 TeV. Its main objectives are precise top quark, Higgs boson and Beyond Standard Model physics. In addition to spatial resolutions of a few micrometers and a…

Instrumentation and Detectors · Physics 2021-03-10 Simon Spannagel

Microcalorimeter instruments aboard future X-ray observatories will require an anti-coincidence (anti-co) detector to veto charged particle events and reduce the non-X-ray background. We have developed a large-format, TES-based prototype…

The Gamma Ray Large Area Space Telescope (GLAST) Large Area Telescope (LAT) is a pair-production high-energy (>20 MeV) gamma-ray telescope being built by an international partnership of astrophysicists and particle physicists for a…

The new beam profile measurement for the Antiproton Decelerator (AD) at CERN is based on a single Gas Electron Multiplier (GEM) with a 2D readout structure. This detector is very light (~0.4% X0), and measures horizontal and vertical…

Instrumentation and Detectors · Physics 2012-03-20 Serge Duarte Pinto , Rhodri Jones , Leszek Ropelewski , Jens Spanggaard , Gerard Tranquille

COCOA (COmpact COmpton cAmera) is a next-generation gamma-ray telescope designed for astrophysical observations in the MeV energy range. The detector comprises a scatterer volume employing the LiquidO detection technology and an array of…

The High Granularity Timing Detector (HGTD) will be installed in the ATLAS experiment as part of the Phase-II upgrade for the High Luminosity-Large Hadron Collider (HL-LHC). It will mitigate pile-up effects in the forward region, and…

Instrumentation and Detectors · Physics 2026-02-02 A. Aboulhorma , M. Ait Tamlihat , H. M. Alfanda , O. Atanova , N. Atanov , I. Azzouzi , J. Barreiro Guimarães da Costa , T. Beau , D. Benchekroun , F. Bendebba , G. Bergamin , Y. Bimgdi , A. Blot , A. Boikov , J. Bonis , D. Boumediene , C. Brito , A. S. Brogna , A. M. Burger , L. Cadamuro , Y. Cai , N. Cartalade , R. Casanova Mohr , R. Cherkaoui El Moursli , Y. Che , X. Chen , E. Y. S. Chow , L. D. Corpe , C. G. Crozatier , L. D'Eramo , S. Dahbi , D. Dannheim , G. Daubard , Y. Davydov , J. Debevc , Y. Degerli , E. Delagnes , F. Deliot , M. Dhellot , P. Dinaucourt , G. Di Gregorio , P. J. Dos Santos De Assis , C. Duan , O. Duarte , F. Dulucq , J. Ehrecke , Y. El Ghazali , A. El Moussaouy , A. Falou , L. Fan , Y. Fan , Z. Fan , K. Farman , F. Fassi , Y. Feng , M. Ferreira , F. Filthaut , F. Fischer , P. Fusté , J. Fu , J. García Rodriquez , G. Gaspar De Andrade , V. Gautam , Z. Ge , R. Gonçalo , M. Gouighri , S. Grinstein , K. Gritsay , F. Guilloux , S. Guindon , A. Haddad , S. E. D. Hammoud , L. Han , A. M. Henriques Correia , M. Hidaoui , B. Hiti , J. Hofner , S. Hou , P. J. Hsu , X. Huang , Y. Huang , K. Hu , C. Insa , J. Jeglot , X. Jia , G. Kramberger , M. Kuriyama , B. Y. Ky , D. Lacour , A. Lafarge , B. Lakssir , A. Lantheaume , D. Laporte , C. de La Taille , M. A. L. Leite , A. Leopold , H. Li , L. Li , M. Li , S. Li , S. Li , Y. Li , Z. Li , S. Liang , Z. Liang , B. Liu , K. Liu , K. Liu , Y. L. Liu , Y. W. Liu , F. L. Lucio Alves , M. Lu , Y. J. Lu , F. Lyu , D. Macina , R. Madar , N. Makovec , S. Malyukov , I. Mandić , T. Manoussos , S. Manzoni , G. Martin-Chassard , F. Martins , L. Masetti , R. Mazini , E. Mazzeo , K. Ma , X. Ma , R. Menegasso , J-P. Meyer , Y. Miao , A. Migayron , M. Mihovilovic , M. Milovanovic , M. Missio , V. Moskalenko , N. Mouadili , A. Moussa , I. Nikolic-Audit , C. C. Ohm , H. Okawa , S. Okkerman , M. Ouchrif , C. Pénélaud , A. Parreira , B. Pascual Dias , R. E. de Paula , J. Pinol Bel , P. -O. Puhl , C. Puigdengoles Olive , M. Puklavec , J. Qin , M. Qi , H. Ren , H. Riani , S. Ridouani , V. Rogozin , L. Royer , F. Rudnyckyj , E. F. Saad , G. T. Saito , A. Salem , H. Santos , S. Scarfi , Ph. Schwemling , N. Seguin-Moreau , L. Serin , R. P. Serrano Fernandez , A. Shaikovskii , Q. Sha , L. Shan , R. Shen , X. Shi , P. Skomina , H. Smitmanns , H. L. Snoek , A. P. Soulier , A. Stein , H. Stenzel , J. Strandberg , W. Sun , X. Sun , Y. Sun , Y. Tan , K. Tariq , Y. Tayalati , S. Terzo , A. Torrento Coello , S. Trincaz-Duvoid , U. M. Vande Voorde , I. Velkovska , R. P. Vieira , L. A. Vieira Lopes , A. Visibile , A. Wang , C. Wang , S. M. Wang , T. Wang , T. Wang , W. Wang , Y. Wang , Y. Wang , J. Wan , Q. Weitzel , J. Wu , M. Wu , W. Wu , Y. Wu , L. Xia , D. Xu , H. Xu , L. Xu , Z. Yan , H. Yang , H. Yang , X. Yang , X. Yang , J. Ye , I. Youbi , J. Yuan , I. Zahir , H. Zeng , D. Zhang , J. Zhang , L. Zhang , Z. Zhang , M. Zhao , Z. Zhao , X. Zheng , Z. Zhou , Y. Zhu , X. Zhuang

The Crystal Barrel is an electromagnetic calorimeter consisting of 1380 CsI(Tl) scintillators, and is currently installed at the CBELSA/TAPS experiment where it is used to detect decay products from photoproduction of mesons. The readout of…

Skipper Charge-Coupled Devices (skipper-CCDs) are pixelated silicon detectors with deep sub-electron resolution. Their radiation hardness and capability to reconstruct energy deposits with unprecedented precision make them a promising…

Instrumentation and Methods for Astrophysics · Physics 2026-05-11 Ana M. Botti , Yikai Wu , Brenda Cervantes , Claudio Chavez , Juan Estrada , Stephen E. Holland , Nathan Saffold , Javier Tiffenberg , Sho Uemura

An advanced Compton telescope appears to be the best instrument concept for the next generation gamma-ray space observatory in the MeV range. A first prototype of advanced Compton telescope is being developed to match the constraints of a…

Instrumentation and Methods for Astrophysics · Physics 2020-02-27 Adrien Laviron , Valentin Gourlaouen , Clarisse Hamadache , Corentin Hiver , Jürgen Kiener , Jean Peyré , Vincent Tatischeff

A future mission in medium-energy gamma-ray astrophysics would allow for many scientific advancements, e.g. a possible explanation for the excess positron emission from the Galactic Center, a better understanding of nucleosynthesis and…

Instrumentation and Methods for Astrophysics · Physics 2018-06-20 Michelle Galloway , Andreas Zoglauer , Steven E. Boggs , Mark Amman

Charge Coupled Devices (CCDs) have been successfully used in several high energy physics experiments over the past two decades. Their high spatial resolution and thin sensitive layers make them an excellent tool for studying short-lived…

A prototype detector is being developed which combines the functions of a Time Projection Chamber for charged particle tracking and a Cherenkov detector for particle identification. The TPC consists of a 10x10x10 cm3 drift volume where the…

Instrumentation and Detectors · Physics 2015-12-18 Craig Woody , Babak Azmoun , Richard Majka , Michael Phipps , Martin Purschke , Nikolai Smirnov

A Compton camera is the most promising approach for gamma-ray detection in the energy region from several hundred keV to MeV, especially for application in high energy astrophysics. In order to obtain good angular resolution, semiconductor…

In this paper we present the R&D activity on a new GEM-based TPC prototype for AMADEUS, a new experimental proposal at the DA{\Phi}NE {\Phi}-factory at the Laboratori Nazionali di Frascati (INFN), aiming to perform measurements of the…

Instrumentation and Detectors · Physics 2013-04-24 M. Poli Lener , M. Bazzi , G. Corradi , C. Curceanu , A. D'Uffizi , C. Paglia , E. Sbardella , A. Scordo , D. Tagnani , A. Romero Vidal , J. Zmeskal

We present a candidate sensor for future spectroscopic applications, such as a Stage-5 Spectroscopic Survey Experiment or the Habitable Worlds Observatory. This type of charge-coupled device (CCD) sensor features multiple in-line amplifiers…

X-Calibur is a balloon-borne telescope that measures the polarization of high-energy X-rays in the 15--50keV energy range. The instrument makes use of the fact that X-rays scatter preferentially perpendicular to the polarization direction.…

The key component of the future PANDA experiment at FAIR is a fixed-target detector for collisions of antiprotons with a proton target up to a beam momentum of 15 GeV/c and is designed to address a large number of open questions in the…

We have developed large-area lithium-drifted silicon (Si(Li)) detectors to meet the unique requirements of the General Antiparticle Spectrometer (GAPS) experiment. GAPS is an Antarctic balloon-borne mission scheduled for the first flight in…

Instrumentation and Methods for Astrophysics · Physics 2018-12-19 M. Kozai , H. Fuke , M. Yamada , T. Erjavec , C. J. Hailey , C. Kato , N. Madden , K. Munakata , K. Perez , F. Rogers , N. Saffold , Y. Shimizu , K. Tokuda , M. Xiao

The past ten years have seen the advent of silicon-based precise timing detectors for charged particle tracking. The underlying reason for this evolution is a design innovation: the Low-Gain Avalanche Diode (LGAD). In its simplicity, the…

High Energy Physics - Experiment · Physics 2022-08-31 N. Cartiglia , R. Arcidiacono , M. Costa , M. Ferrero , G. Gioachin , M. Mandurrino , L. Menzio , F. Siviero , V. Sola , M. Tornago