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The Multigap Resistive Plate Chambers (MRPC) are used as a timing detector in several particle physics and cosmic ray experiments. The gas mixture of MRPC at current experiments is a mixture containing $\rm C_2F_4H_2$ and in some cases $\rm…

Instrumentation and Detectors · Physics 2020-01-29 Baek Yongwook , Kim Do-won , Park Woosung , Williams Crispin , Zuyeuski Roman

A current focus at RHIC is the Beam Energy Scan to study the QCD phase diagram -- temperature ($T$) vs. baryon chemical potential ($\mu_{B}$). The STAR experiment has collected data for Au+Au collisions at $\sqrt{s_{NN}}=$ 7.7 GeV, 11.5…

Nuclear Experiment · Physics 2015-05-28 Lokesh Kumar

The search for neutrinoless double beta decay requires increasingly advanced methods of background reduction. A bold approach to solving this problem, in experiments using Xe-136, is to extract and identify the daughter Ba-136 ion produced…

Instrumentation and Detectors · Physics 2019-10-07 K. Murray , J. Dilling , R. Gornea , Y. Ito , T. Koffas , A. A. Kwiatkowski , Y. Lan , M. P. Reiter , V. Varentsov , T. Brunner

The CMS experiment, located at the CERN Large Hadron Collider, has a redundant muon system composed by three different detector technologies: Cathode Strip Chambers (in the forward regions), Drift Tubes (in the central region) and Resistive…

The aim of this work is to show the potential capabilities of monolithic crystals coupled to large SiPM arrays, to be considered as detector blocks for PET scanners enabling Time Of Flight (TOF) capabilities. Monolithic blocks allow one to…

PANDA (anti-Proton ANnihiliation at DArmstadt) is planned to be one of the four main experiments at the future international accelerator complex FAIR (Facility for Antiproton and Ion Research) in Darmstadt, Germany. It is going to address…

Instrumentation and Detectors · Physics 2020-01-01 Panda Collaboration , F. Davi , W. Erni , B. Krusche , M. Steinacher , N. Walford , H. Liu , Z. Liu , B. Liu , X. Shen , C. Wang , J. Zhao , M. Albrecht , T. Erlen , F. Feldbauer , M. Fink , V. Freudenreich , M. Fritsch , F. H. Heinsius , T. Held , T. Holtmann , I. Keshk , H. Koch , B. Kopf , M. Kuhlmann , M. Kümmel , S. Leiber , P. Musiol , A. Mustafa , M. Pelizäus , A. Pitka , G. Reicherz , M. Richter , C. Schnier , T. Schröder , S. Sersin , L. Sohl , C. Sowa , M. Steinke , T. Triffterer , U. Wiedner , R. Beck , C. Hammann , J. Hartmann , B. Ketzer , M. Kube , M. Rossbach , C. Schmidt , R. Schmitz , U. Thoma , M. Urban , A. Bianconi , M. Bragadireanu , D. Pantea , W. Czyzycki , M. Domagala , G. Filo , J. Jaworowski , M. Krawczyk , E. Lisowski , F. Lisowski , M. Michalek , J. Plazek , K. Korcyl , A. Kozela , P. Kulessa , P. Lebiedowicz , K. Pysz , W. Schäfer , A. Szczurek , T. Fiutowski , M. Idzik , B. Mindur , K. Swientek , J. Biernat , B. Kamys , S. Kistryn , G. Korcyl , W. Krzemien , A. Magiera , P. Moskal , W. Przygoda , Z. Rudy , P. Salabura , J. Smyrski , P. Strzempek , A. Wronska , I. Augustin , R. Böhm , I. Lehmann , D. Nicmorus Marinescu , L. Schmitt , V. Varentsov , M. Al-Turany , A. Belias , H. Deppe , N. Divani Veis , R. Dzhygadlo , H. Flemming , A. Gerhardt , K. Götzen , R. Karabowicz , U. Kurilla , D. Lehmann , S. Löchner , J. Lühning , U. Lynen , S. Nakhoul , H. Orth , K. Peters , T. Saito , G. Schepers , C. J. Schmidt , C. Schwarz , J. Schwiening , A. Täschner , M. Traxler , B. Voss , P. Wieczorek , A. Wilms , V. Abazov , G. Alexeev , V. A. Arefiev , V. Astakhov , M. Yu. Barabanov , B. V. Batyunya , V. Kh. Dodokhov , A. Efremov , A. Fechtchenko , A. Galoyan , G. Golovanov , E. K. Koshurnikov , Y. Yu. Lobanov , V. I. Lobanov , V. Malyshev , A. G. Olshevskiy , A. A. Piskun , A. Samartsev , M. G. Sapozhnikov , N. B. Skachkov , A. N. Skachkova , E. A. Strokovsky , V. Tokmenin , V. Uzhinsky , A. Verkheev , A. Vodopianov , N. I. Zhuravlev , A. Zinchenko , D. Branford , D. Glazier , D. Watts , M. Böhm , W. Eyrich , A. Lehmann , D. Miehling , M. Pfaffinger , S. Stelter , F. Uhlig , S. Dobbs , K. Seth , A. Tomaradze , T. Xiao , D. Bettoni , A. Ali , A. Hamdi , M. Krebs , F. Nerling , V. Akishina , S. Gorbunov , I. Kisel , G. Kozlov , M. Pugach , M. Zyzak , N. Bianchi , P. Gianotti , C. Guaraldo , V. Lucherini , G. Bracco , S. Bodenschatz , K. T. Brinkmann , V. Di Pietro , S. Diehl , V. Dormenev , M. Düren , E. Etzelmüller , K. Föhl , M. Galuska , T. Geßler , E. Gutz , C. Hahn , A. Hayrapetyan , M. Kesselkaul , W. Kühn , T. Kuske , J. S. Lange , Y. Liang , V. Metag , M. Moritz , M. Nanova , R. Novotny , T. Quagli , A. Riccardi , J. Rieke , M. Schmidt , R. Schnell , H. Stenzel , M. Strickert , U. Thöring , T. Wasem , B. Wohlfahrt , H. G. Zaunick , E. Tomasi-Gustafsson , D. Ireland , G. Rosner , B. Seitz , P. N. Deepak , A. Kulkarni , A. Apostolou , M. Babai , M. Kavatsyuk , H. Loehner , J. Messchendorp , P. Schakel , M. Tiemens , J. C. van der Weele , S. Vejdani , K. Dutta , K. Kalita , H. Sohlbach , M. Bai , L. Bianchi , M. Büscher , A. Derichs , R. Dosdall , A. Erven , V. Fracassi , A. Gillitzer , F. Goldenbaum , D. Grunwald , L. Jokhovets , G. Kemmerling , H. Kleines , A. Lai , A. Lehrach , M. Mikirtychyants , S. Orfanitski , D. Prasuhn , E. Prencipe , J. Pütz , J. Ritman , E. Rosenthal , S. Schadmand , T. Sefzick , V. Serdyuk , G. Sterzenbach , T. Stockmanns , P. Wintz , P. Wüstner , H. Xu , Y. Zhou , Z. Li , X. Ma , H. Xu , V. Rigato , L. Isaksson , P. Achenbach , A. Aycock , O. Corell , A. Denig , M. Distler , M. Hoek , W. Lauth , Z. Liu , H. Merkel , U. Müller , J. Pochodzalla , S. Sanchez , S. Schlimme , C. Sfienti , M. Thiel , M. Zambrana , H. Ahmadi , S. Ahmed , S. Bleser , L. Capozza , M. Cardinali , A. Dbeyssi , A. Ehret , B. Fröhlich , P. Grasemann , S. Haasler , D. Izard , J. Jorge , D. Khaneft , R. Klasen , R. Kliemt , J. Köhler , H. H. Leithoff , D. Lin , F. Maas , S. Maldaner , M. Michel , M. C. Mora Espi , C. Morales Morales , C. Motzko , O. Noll , S. Pflüger , D. Rodriguez Pineiro , M. Steinen , E. Walaa , S. Wolff , I. Zimmermann , A. Fedorov , M. Korzhik , O. Missevitch , P. Balanutsa , V. Chernetsky , A. Demekhin , A. Dolgolenko , P. Fedorets , A. Gerasimov , V. Goryachev , D. Y. Kirin , V. A. Matveev , A. V. Stavinskiy , A. Balashoff , A. Boukharov , O. Malyshev , I. Marishev , V. Chandratre , V. Datar , V. Jha , H. Kumawat , A. K. Mohanty , A. Parmar , A. K. Rai , B. Roy , G. Sonika , C. Fritzsch , S. Grieser , A. K. Hergemöller , B. Hetz , N. Hüsken , A. Khoukaz , J. P. Wessels , C. Herold , K. Khosonthongkee , C. Kobdaj , A. Limphirat , P. Srisawad , Y. Yan , A. E. Blinov , S. Kononov , E. A. Kravchenko , E. Antokhin , M. Barnyakov , A. Yu. Barnyakov , K. Beloborodov , V. E. Blinov , V. S. Bobrovnikov , I. A. Kuyanov , A. P. Onuchin , S. Pivovarov , E. Pyata , S. Serednyakov , Y. Tikhonov , R. Kunne , D. Marchand , B. Ramstein , J. van de Wiele , Y. Wang , G. Boca , V. Burian , M. Finger , M. Finger , A. Nikolovova , M. Pesek , M. Peskova , M. Pfeffer , I. Prochazka , M. Slunecka , P. Gallus , V. Jary , J. Novy , M. Tomasek , M. Virius , V. Vrba , V. Abramov , N. Belikov , S. Bukreeva , A. Davidenko , A. Derevschikov , Y. Goncharenko , V. Grishin , V. Kachanov , V. Kormilitsin , A. Levin , Y. Melnik , N. Minaev , V. Mochalov , D. Morozov , L. Nogach , S. Poslavskiy , A. Ryazantsev , S. Ryzhikov , P. Semenov , I. Shein , A. Uzunian , A. Vasiliev , A. Yakutin , U. Roy , B. Yabsley , S. Belostotski , G. Gavrilov , A. Izotov , S. Manaenkov , O. Miklukho , D. Veretennikov , A. Zhdanov , T. Bäck , B. Cederwall , K. Makonyi , M. Preston , P. E. Tegner , D. Wölbing , S. Godre , M. P. Bussa , S. Marcello , S. Spataro , F. Iazzi , R. Introzzi , A. Lavagno , D. Calvo , P. De Remigis , A. Filippi , G. Mazza , A. Rivetti , R. Wheadon , A. Martin , H. Calen , W. Ikegami Andersson , T. Johansson , A. Kupsc , P. Marciniewski , M. Papenbrock , J. Pettersson , J. Regina , K. Schönning , M. Wolke , J. Diaz , V. Pothodi Chackara , A. Chlopik , G. Kesik , D. Melnychuk , B. Slowinski , A. Trzcinski , M. Wojciechowski , S. Wronka , B. Zwieglinski , P. Bühler , J. Marton , D. Steinschaden , K. Suzuki , E. Widmann , S. Zimmermann , J. Zmeskal

Experiments with low-energy antiprotons are currently performed at the Antiproton Decelerator of CERN. The main experiments deal with the spectroscopy of antiprotonic helium, an exotic three-body system, and the formation and spectroscopy…

High Energy Physics - Experiment · Physics 2010-03-09 E. Widmann

The Muon Upgrade Phase II of the Compact Muon Solenoid (CMS) aims to guarantee the optimal conditions of the present system and extend the $\eta$ coverage to ensure a reliable system for the High Luminosity Large Hadron Collider (HL-LHC)…

Instrumentation and Detectors · Physics 2020-06-17 M. I. Pedraza-Morales

Multi-reflection time-of-flight mass separators and spectrometers (MR-ToF MSs) are indispensable tools at radioactive ion beam (RIB) facilities. These electrostatic ion beam traps act as highly selective mass separators and high-precision…

The Multi-gap Resistive Plate Chamber (MRPC) is an advanced form of Resistive Plate Chamber (RPC) detector where the gas gap is divided into sub-gaps. MRPCs are known for their good time resolution and detection efficiency for charged…

Instrumentation and Detectors · Physics 2018-08-15 Rajesh Ganai , Mitali Mondal , Shaifali Mehta , Zubayer Ahammed , Subhasis Chattopadhyay

The MIMAC project is multi-chamber detector for Dark Matter search, aiming at measuring both track and ionization with a matrix of micromegas micro-TPC filled with He3 and CF4. Recent experimental results on the first measurements of the…

Cosmology and Nongalactic Astrophysics · Physics 2010-11-02 F. Mayet , O. Guillaudin , D. Santos , A. Trichet

A new prototype of large area Multi-gap Resistive Plate Chamber (MRPC) with long readout strips was built. This Long-strip Multi-gap Resistive Plate Chamber (LMRPC) is double stacked and has ten 250 $\mu$m-thick gas gaps. Signals are read…

Instrumentation and Detectors · Physics 2015-05-20 Yongjie sun , Cheng Li , Zebo Tang , Lailin Xu , Tianxiang Chen , Ming Shao

The exploration of the QCD phase diagram has been one of the main drivers of contemporary nuclear physics. The Relativistic Heavy Ion Collider (RHIC) at BNL is uniquely suited for this task through its Beam Energy Scan (BES) program which…

Nuclear Experiment · Physics 2018-10-12 David Tlusty

We constructed a new time-of-flight (TOF) detector consisting of resistive plate chambers (RPCs) to measure particle energy in the BGOegg experiment. The BGOegg-RPC has a unique feature which enables us to cover a large area with a small…

Instrumentation and Detectors · Physics 2016-12-21 N. Tomida , N. Tran , M. Niiyama , H. Ohnishi , N. Muramatsu

The Beam Dump Facility (BDF) project is a proposed general-purpose facility at CERN, dedicated to beam dump and fixed target experiments. In its initial phase, the facility is foreseen to be exploited by the Search for Hidden Particles…

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…

This paper discusses a detailed design approach to determine the optimal input impedance (Rin) and bandwidth (BW) for current preamplifiers in Front End Electronics (FEE) of high-accuracy time measurement systems used in particle detection.…

Instrumentation and Detectors · Physics 2021-04-29 Abderrahmane Ghimouz , Fatah Rarbi , Olivier Rossetto

We have developed multi-gap resistive plate chambers (MRPCs) with 2.5 x 200 cm2 readout strips for the time-of-flight (TOF) detector system of the LEPS2 experiment at SPring-8. These chambers consist of 2 stacks and 5 gas gaps per stack, in…

Transition Edge Sensor (TES) bolometers are a well-established technology with a strong track record in experimental cosmology, making them ideal for current and future radio astronomy instruments. The Tomographic Ionized-carbon Mapping…

Instrumentation and Methods for Astrophysics · Physics 2025-10-06 Victoria L. Butler , James J. Bock , Dongwoo T. Chung , Abigail T. Crites , King Lau , Ian Lowe , Dan P. Marrone , Evan C. Mayer , Benjamin J. Vaughan , Michael Zemcov

A Cosmic Ray Test Facility (CRTF) is the first large-scale implementation of a scintillation triggering system based on a new scintillation technique known as START. In START, the scintillation light is collected and transported by WLS…

Instrumentation and Detectors · Physics 2009-11-13 A. Akindinov , V. Golovin , E. Grigoriev , Yu. Grishuk , S. Kuleshov , D. Malkevich , A. Martemiyanov , A. Nedosekin , M. Ryabinin , K. Voloshin