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The Short Baseline Near Detector (SBND) is one of three liquid argon (LAr) neutrino detectors sitting in the Booster Neutrino Beam (BNB) at Fermilab as part of the Short Baseline Neutrino (SBN) program. The detector is in a cryostat holding…

Instrumentation and Detectors · Physics 2019-10-16 Shanshan Gao

In this paper we describe how the readout planes for the MicroBooNE Time Projection Chamber were constructed, assembled and installed. We present the individual wire preparation using semi-automatic winding machines and the assembly of wire…

Single photon avalanche diode (SPAD) arrays have proven themselves as serious candidates for time of flight positron emission tomography (PET). Discrete readout schemes mitigate the low-noise requirements of analog schemes and offer very…

Instrumentation and Detectors · Physics 2018-06-28 M. -A. Tétrault , É. Desaulniers Lamy , A. Boisvert , C. Thibaudeau , F. Dubois , R. Fontaine , J. -F. Pratte

The Short-Baseline Near Detector (SBND) is one of three Liquid Argon Time Projection Chamber (LArTPC) neutrino detectors positioned along the axis of the Booster Neutrino Beam (BNB) at Fermilab, as part of the Short-Baseline Neutrino (SBN)…

High Energy Physics - Experiment · Physics 2025-01-22 Rodrigo Alvarez Garrote

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

The low-noise operation of readout electronics in a liquid argon time projection chamber (LArTPC) is critical to properly extract the distribution of ionization charge deposited on the wire planes of the TPC, especially for the induction…

Instrumentation and Detectors · Physics 2023-02-17 MicroBooNE collaboration , R. Acciarri , C. Adams , R. An , J. Anthony , J. Asaadi , M. Auger , L. Bagby , S. Balasubramanian , B. Baller , C. Barnes , G. Barr , M. Bass , F. Bay , M. Bishai , A. Blake , T. Bolton , B. Bullard , L. Camilleri , D. Caratelli , B. Carls , R. Castillo Fernandez , F. Cavanna , H. Chen , E. Church , D. Cianci , E. Cohen , G. H. Collin , J. M. Conrad , M. Convery , J. I. Crespo-Anadon , G. De Geronimo , M. Del Tutto , D. Devitt , S. Dytman , B. Eberly , A. Ereditato , L. Escudero Sanchez , J. Esquivel , A. A. Fadeeva , B. T. Fleming , W. Foreman , A. P. Furmanski , D. Garcia-Gamez , G. T. Garvey , V. Genty , D. Goeldi , S. Gollapinni , N. Graf , E. Gramellini , H. Greenlee , R. Grosso , R. Guenette , A. Hackenburg , P. Hamilton , O. Hen , V Hewes , C. Hill , J. Ho , G. Horton-Smith , A. Hourlier , E. -C. Huang , C. James , J. Jan de Vries , C. -M. Jen , L. Jiang , R. A. Johnson , J. Joshi , H. Jostlein , D. Kaleko , G. Karagiorgi , W. Ketchum , B. Kirby , M. Kirby , T. Kobilarcik , I. Kreslo , A. Laube , S. Li , Y. Li , A. Lister , B. R. Littlejohn , S. Lockwitz , D. Lorca , W. C. Louis , M. Luethi , B. Lundberg , X. Luo , A. Marchionni , C. Mariani , J. Marshall , D. A. Martinez Caicedo , V. Meddage , T. Miceli , G. B. Mills , J. Moon , M. Mooney , C. D. Moore , J. Mousseau , R. Murrells , D. Naples , P. Nienaber , J. Nowak , O. Palamara , V. Paolone , V. Papavassiliou , S. F. Pate , Z. Pavlovic , E. Piasetzky , D. Porzio , G. Pulliam , X. Qian , J. L. Raaf , V. Radeka , A. Rafique , S. Rescia , L. Rochester , C. Rudolf von Rohr , B. Russell , D. W. Schmitz , A. Schukraft , W. Seligman , M. H. Shaevitz , J. Sinclair , A. Smith , E. L. Snider , M. Soderberg , S. Soldner-Rembold , S. R. Soleti , P. Spentzouris , J. Spitz , J. St. John , T. Strauss , A. M. Szelc , N. Tagg , K. Terao , M. Thomson , C. Thorn , M. Toups , Y. -T. Tsai , S. Tufanli , T. Usher , W. Van De Pontseele , R. G. Van de Water , B. Viren , M. Weber , D. A. Wickremasinghe , S. Wolbers , T. Wongjirad , K. Woodruff , T. Yang , L. Yates , B. Yu , G. P. Zeller , J. Zennamo , C. Zhang

In the Large High Altitude Air Shower Observatory (LHAASO), the Water Cherenkov Detector Array (WCDA) is one of the key parts. The WCDA consists of 3600 Photomultiplier Tubes (PMTs) scattered in a 90000 m2 area, and both high precision time…

Instrumentation and Detectors · Physics 2019-08-06 Lei Zhao , Cong Ma , Shaoping Chu , Xingshun Gao , Zouyi Jiang , Ruoshi Dong , Shubin Liu , Qi An

Micro-Pattern Gaseous Detectors (MPGDs) with resistive anode planes provide intrinsic discharge robustness while maintaining good spatial and time resolutions. Typically read out with 1D strips or pad structures, here the characterisation…

Generally, a superconducting nanowire single-photon detector (SNSPD) is composed of wires with a typical width of ~100 nm. Recent studies have found that superconducting strips with a micrometer-scale width can also detect single photons.…

Instrumentation and Detectors · Physics 2021-04-28 Guang-Zhao Xu , Wei-Jun Zhang , Li-Xing You , Jia-Min Xiong , Xing-Qu Sun , Hao Huang , Xin Ou , Yi-Ming Pan , Chao-Lin Lv , Hao Li , Zhen Wang , Xiao-Ming Xie

A normal pressure MWPC for beam diagnostics at RIBLL2 has been developed, which has a sensitive area of 80 mm$\times$80 mm and consists of three-layer wire planes. The anode plane is designed with a wider frame to reduce the discharge and…

Instrumentation and Detectors · Physics 2015-06-16 Shu-Wen Tang , Peng Ma , Li-Min Duan , Zhi-Yu Sun , Chen-Gui Lu , He-Run Yang , Rong-Jiang Hu , Wen-Xue Huang , Hu-Shan Xu

We report on studies of fast triggering and high-precision tracking using Resistive Plate Chambers (RPCs). Two beam tests were carried out with the 180 GeV muon beam at CERN using RPCs with gas gaps of 1.00 or 1.15 mm and equipped with…

This paper describes the small-diameter monitored drift-tube detector construction at the University of Michigan as a contribution to the ATLAS Muon Spectrometer upgrade for the high-luminosity Large Hadron Collider at CERN. Measurements of…

We present a characterization of a small (9-liter) and mobile 0.1% 6Li-doped pulse-shape-sensitive plastic scintillator antineutrino detector called SANDD (Segmented AntiNeutrino Directional Detector), constructed for the purpose of…

Instrumentation and Detectors · Physics 2021-06-02 F. Sutanto , T. M. Classen , S. A. Dazeley , M. J. Duvall , I. Jovanovic , V. A. Li , A. N. Mabe , E. T. E. Reedy , T. Wu

This paper describes the design and construction of the MicroBooNE liquid argon time projection chamber and associated systems. MicroBooNE is the first phase of the Short Baseline Neutrino program, located at Fermilab, and will utilize the…

Instrumentation and Detectors · Physics 2023-02-17 MicroBooNE Collaboration , R. Acciarri , C. Adams , R. An , A. Aparicio , S. Aponte , J. Asaadi , M. Auger , N. Ayoub , L. Bagby , B. Baller , R. Barger , G. Barr , M. Bass , F. Bay , K. Biery , M. Bishai , A. Blake , V. Bocean , D. Boehnlein , V. D. Bogert , T. Bolton , L. Bugel , C. Callahan , L. Camilleri , D. Caratelli , B. Carls , R. Castillo Fernandez , F. Cavanna , S. Chappa , H. Chen , K. Chen , C. Y. Chi , C. S. Chiu , E. Church , D. Cianci , G. H. Collin , J. M. Conrad , M. Convery , J. Cornele , P. Cowan , J. I. Crespo-Anadon , G. Crutcher , C. Darve , R. Davis , M. Del Tutto , D. Devitt , S. Duffin , S. Dytman , B. Eberly , A. Ereditato , D. Erickson , L. Escudero Sanchez , J. Esquivel , S. Farooq , J. Farrell , D. Featherston , B. T. Fleming , W. Foreman , A. P. Furmanski , V. Genty , M. Geynisman , D. Goeldi , B. Goff , S. Gollapinni , N. Graf , E. Gramellini , J. Green , A. Greene , H. Greenlee , T. Griffin , R. Grosso , R. Guenette , A. Hackenburg , R. Haenni , P. Hamilton , P. Healey , O. Hen , E. Henderson , V Hewes , C. Hill , K. Hill , L. Himes , J. Ho , G. Horton-Smith , D. Huffman , C. M. Ignarra , C. James , E. James , J. Jan de Vries , W. Jaskierny , C. M. Jen , L. Jiang , B. Johnson , M. Johnson , R. A. Johnson , B. J. P. Jones , J. Joshi , H. Jostlein , D. Kaleko , L. N. Kalousis , G. Karagiorgi , T. Katori , P. Kellogg , W. Ketchum , J. Kilmer , B. King , B. Kirby , M. Kirby , E. Klein , T. Kobilarcik , I. Kreslo , R. Krull , R. Kubinski , G. Lange , F. Lanni , A. Lathrop , A. Laube , W. M. Lee , Y. Li , D. Lissauer , A. Lister , B. R. Littlejohn , S. Lockwitz , D. Lorca , W. C. Louis , G. Lukhanin , M. Luethi , B. Lundberg , X. Luo , G. Mahler , I. Majoros , D. Makowiecki , A. Marchionni , C. Mariani , D. Markley , J. Marshall , D. A. Martinez Caicedo , K. T. McDonald , D. McKee , A. McLean , J. Mead , V. Meddage , T. Miceli , G. B. Mills , W. Miner , J. Moon , M. Mooney , C. D. Moore , Z. Moss , J. Mousseau , R. Murrells , D. Naples , P. Nienaber , B. Norris , N. Norton , J. Nowak , M. OBoyle , T. Olszanowski , O. Palamara , V. Paolone , V. Papavassiliou , S. F. Pate , Z. Pavlovic , R. Pelkey , M. Phipps , S. Pordes , D. Porzio , G. Pulliam , X. Qian , J. L. Raaf , V. Radeka , A. Rafique , R. A Rameika , B. Rebel , R. Rechenmacher , S. Rescia , L. Rochester , C. Rudolf von Rohr , A. Ruga , B. Russell , R. Sanders , W. R. Sands , M. Sarychev , D. W. Schmitz , A. Schukraft , R. Scott , W. Seligman , M. H. Shaevitz , M. Shoun , J. Sinclair , W. Sippach , T. Smidt , A. Smith , E. L. Snider , M. Soderberg , M. Solano-Gonzalez , S. Soldner-Rembold , S. R. Soleti , J. Sondericker , P. Spentzouris , J. Spitz , J. St. John , T. Strauss , K. Sutton , A. M. Szelc , K. Taheri , N. Tagg , K. Tatum , J. Teng , K. Terao , M. Thomson , C. Thorn , J. Tillman , M. Toups , Y. T. Tsai , S. Tufanli , T. Usher , M. Utes , R. G. Van de Water , C. Vendetta , S. Vergani , E. Voirin , J. Voirin , B. Viren , P. Watkins , M. Weber , T. Wester , J. Weston , D. A. Wickremasinghe , S. Wolbers , T. Wongjirad , K. Woodruff , K. C. Wu , T. Yang , B. Yu , G. P. Zeller , J. Zennamo , C. Zhang , M. Zuckerbrot

A prototype of Multi-Wire Proportional Chambers (MWPC) has been fabricated for the study of its various characteristics. The detector contains gold-coated tungsten wires (20 $\mu m$ diameter) on the anode frame, with a pitch of 2.8 mm. The…

Instrumentation and Detectors · Physics 2021-10-06 Rajendra Nath Patra , R. N. Singaraju , S. Biswas , T. K. Nayak , Y. P. Viyogi

Down-scaling device dimensions to the nanometer range raises significant challenges to traditional device design, due to potential current leakage across nanoscale dimensions and the need to maintain reproducibility while dealing with…

Mesoscale and Nanoscale Physics · Physics 2019-01-03 Zhongcan Xiao , Chuanxu Ma , Jingsong Huang , Liangbo Liang , Wenchang Lu , Kunlun Hong , Bobby G. Sumpter , An-Ping Li , J. Bernholc

The Short Baseline Near Detector (SBND) is a 112 ton active mass liquid argon time projection chamber (LArTPC) that will begin operations in the Booster Neutrino Beamline at Fermilab in 2020. Its main physics goals include high-statistics…

Instrumentation and Detectors · Physics 2019-10-21 Georgia Karagiorgi

An optimized design of a neutron detector based on timing RPCs (Resistive Plate Chambers) with boron-10 neutron converters is presented. The detector is composed of a stack of ten double gap RPCs with aluminium cathode plates coated on both…

Instrumentation and Detectors · Physics 2023-05-03 L. M. S. Margato , G. Canezin , A. Morozov , A. Blanco , J. Saraiva , L. Lopes , P. Fonte

Short Baseline Near Detector (SBND), which is a 260-ton LAr TPC as near detector in Short Baseline Neutrino (SBN) program, consists of 11,264 TPC readout channels. As an enabling technology for noble liquid detectors in neutrino…

Instrumentation and Detectors · Physics 2018-06-26 H. Chen , J. Evans , J. Fried , S. Gao , F. Liu , G. Miller , K. Mistry , J. Pater , A. Szelc , V. Radeka , J. Zhang

One key communication block in 5G and 6G radios is the active phased array (APA). To ensure reliable operation, efficient and timely fault diagnosis of APAs on-site is crucial. To date, fault diagnosis has relied on measurement of frequency…

Signal Processing · Electrical Eng. & Systems 2023-06-08 Martin H. Nielsen , Yufeng Zhang , Changbin Xue , Jian Ren , Yingzeng Yin , Ming Shen , Gert F. Pedersen
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