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Related papers: An FPGA-based Trigger System for CSHINE

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An experiment to measure an invariant mass of {\phi} mesons in nuclear medium is planned as the J-PARC E16 experiment. A trigger merging module (TRG-MRG) has been developed to detect leading-edges from 256 channels of discriminator-output…

Digital off-detector electronics in trigger and data acquisition systems of High-Energy Physics experiments is often implemented by means of SRAM-based FPGAs, which make it possible to achieve reconfigurable, real-time processing and…

Instrumentation and Detectors · Physics 2018-06-29 Raffaele Giordano , Sabrina Perrella , Dario Barbieri , Vincenzo Izzo , Alberto Aloisio

We present a study of the CMS trigger system in heavy-ion collisions. Concentrating on two physics channels, dimuons from decays of quarkonia and single jets, we evaluate a possible trigger strategy for Pb+Pb running that relies on event…

Nuclear Experiment · Physics 2019-08-14 G. Roland

NA61/SHINE (SPS Heavy Ion and Neutrino Experiment) is a multi-purpose experimental facility to study hadron production in hadron-proton, hadron-nucleus and nucleus-nucleus collisions at the CERN Super Proton Synchrotron. It recorded the…

Instrumentation and Detectors · Physics 2014-07-03 N. Abgrall , O. Andreeva , A. Aduszkiewicz , Y. Ali , T. Anticic , N. Antoniou , B. Baatar , F. Bay , A. Blondel , J. Blumer , M. Bogomilov , M. Bogusz , A. Bravar , J. Brzychczyk , S. A. Bunyatov , P. Christakoglou , T. Czopowicz , N. Davis , S. Debieux , H. Dembinski , F. Diakonos , S. DiLuise , W. Dominik , T. Drozhzhova , J. Dumarchez , K. Dynowski , R. Engel , I. Efthymiopoulos , A. Ereditato , A. Fabich , G. A. Feofilov , Z. Fodor , A. Fulop , M. Gazdzicki , M. Golubeva , K. Grebieszkow , A. Grzeszczuk , F. Guber , A. Haesler , T. Hasegawa , M. Hierholzer , R. Idczak , S. Igolkin , A. Ivashkin , D. Jokovic , K. Kadija , A. Kapoyannis , E. Kaptur , D. Kielczewska , M. Kirejczyk , J. Kisiel , T. Kiss , S. Kleinfelder , T. Kobayashi , V. I. Kolesnikov , D. Kolev , V. P. Kondratiev , A. Korzenev , P. Koversarski , S. Kowalski , A. Krasnoperov , A. Kurepin , D. Larsen , A. Laszlo , V. V. Lyubushkin , M. Mackowiak-Pawlowska , Z. Majka , B. Maksiak , A. I. Malakhov , D. Maletic , D. Manglunki , D. Manic , A. Marchionni , A. Marcinek , V. Marin , K. Marton , H. -J. Mathes , T. Matulewicz , V. Matveev , G. L. Melkumov , M. Messina , St. Mrowczynski , S. Murphy , T. Nakadaira , M. Nirkko , K. Nishikawa , T. Palczewski , G. Palla , A. D. Panagiotou , T. Paul , W. Peryt , O. Petukhov , C. Pistillo , R. Planeta , J. Pluta , B. A. Popov , M. Posiadala , S. Pulawski , J. Puzovic , W. Rauch , M. Ravonel , A. Redij , R. Renfordt , E. Richter-Was , A. Robert , D. Rohrich , E. Rondio , B. Rossi , M. Roth , A. Rubbia , A. Rustamov , M. Rybczynski , A. Sadovsky , K. Sakashita , M. Savic , K. Schmidt , T. Sekiguchi , P. Seyboth , D. Sgalaberna , M. Shibata , R. Sipos , E. Skrzypczak , M. Slodkowski , Z. Sosin , P. Staszel , G. Stefanek , J. Stepaniak , H. Stroebele , T. Susa , M. Szuba , M. Tada , V. Tereshchenko , T. Tolyhi , R. Tsenov , L. Turko , R. Ulrich , M. Unger , M. Vassiliou , D. Veberic , V. V. Vechernin , G. Vesztergombi , L. Vinogradov , A. Wilczek , Z. Wlodarczyk , A. Wojtaszek-Szwarz , O. Wyszynski , L. Zambelli , W. Zipper

The Level-1 Muon Barrel Trigger of the ATLAS Experiment at LHC makes use of Resistive Plate Chamber (RPC) detectors. The on-detector trigger electronics modules are able to identify muons with predefined transverse momentum values (pT) by…

Instrumentation and Detectors · Physics 2018-06-27 V. Izzo , A. Aloisio , R. Giordano , S. Perrella , R. Vari

The Gamma Factory (GF) proposal \cite{Krasny:2015ffb} is motivated by the recognition of a largely untapped potential of the CERN accelerator complex to enable a new research programme at the intersection of particle, nuclear, atomic,…

Accelerator Physics · Physics 2026-05-07 Mieczyslaw Witold Krasny

We describe a many-channel experiment control system based on a field-programmable gate array (FPGA). The system has 16 bit resolution on 10 analog 100 MS/s input channels, 14 analog 100 MS/s output channels, 16 slow analog input and output…

Instrumentation and Detectors · Physics 2023-08-03 Daniel T. Schussheim , Kurt Gibble

NA61/SHINE is a multi-purpose experiment to study hadron-proton, hadron-nucleus and nucleus-nucleus collisions at the CERN Super Proton Synchrotron (SPS). The experiment performs unique measurements for the physics of strong interactions as…

Nuclear Experiment · Physics 2020-05-13 Magdalena Kuich

The CMS experiment has been designed with a two-level trigger system: the Level-1 Trigger, implemented on custom-designed electronics, and the High Level Trigger, a streamlined version of the CMS offline reconstruction software running on a…

Instrumentation and Detectors · Physics 2020-11-19 Thiago R. F. P. Tomei

The primary objective of SIRENE is to simulate the response to neutrino events of any type of high energy neutrino telescope. Additionally, it implements different geometries for a neutrino detector and different configurations and…

Increasing luminosity at the Fermilab Tevatron collider has led the D0 collaboration to make improvements to its detector beyond those already in place for Run IIa, which began in March 2001. One of the cornerstones of this Run IIb upgrade…

Instrumentation and Detectors · Physics 2008-11-26 M. Abolins

Machine learning algorithms are being used more frequently in the first-level triggers in collider experiments, with Graph Neural Networks pushing the hardware requirements of FPGA-based triggers beyond the current state of the art. To meet…

High Energy Physics - Experiment · Physics 2026-02-27 Marc Neu , Isabel Haide , Torben Ferber , Jürgen Becker

The determination of charged particle trajectories (tracking) in collisions at the CERN Large Hadron Collider (LHC) is one of the most important aspects for event reconstruction at hadron colliders. This is especially true in the high…

Instrumentation and Detectors · Physics 2022-12-06 H. Abidi , A. Boveia , V. Cavaliere , D. Furletov , A. Gekow , C. W. Kalderon , S. Yoo

The search for experimental signatures of the critical point (CP) of strongly interacting matter is one of the main objectives of the NA61/SHINE experiment at CERN SPS. In the course of the experiment, a beam momentum and system size scan…

Nuclear Experiment · Physics 2020-02-18 Nikolaos Davis

Single muon triggers are crucial for the physics programmes at hadron collider experiments. To be sensitive to electroweak processes, single muon triggers with transverse momentum thresholds down to 20 GeV and dimuon triggers with even…

Instrumentation and Detectors · Physics 2019-03-27 D. Cieri , S. Abovyan , V. Danielyan , M. Fras , P. Gadow , O. Kortner , S. Kortner , H. Kroha , F. Müller , S. Nowak , P. Richter , K. Schmidt-Sommerfeld

We describe a cryogenic instrumentation platform incorporating commercially-available field-programmable gate arrays (FPGAs) configured to operate well beyond their specified temperature range. The instrument enables signal routing,…

Instrumentation and Detectors · Physics 2016-01-20 I. D. Conway Lamb , J. I. Colless , J. M. Hornibrook , S. J. Pauka , S. J. Waddy , M. K. Frechtling , D. J. Reilly

The NA61/SHINE collaboration performed measurements of pC interactions at 31 GeV/c beam momentum with a full size replica of the T2K target (1.9 interaction length) during a pilot run in 2007. Larger statistics runs were also conducted in…

High Energy Physics - Experiment · Physics 2011-11-24 Nicolas Abgrall

The Deep Underground Neutrino Experiment (DUNE) is a next-generation long-baseline neutrino oscillation experiment designed to make precision measurements in the world's most powerful neutrino beam. Neutrinos are measured at two detector…

High Energy Physics - Experiment · Physics 2025-01-28 Ciaran Hasnip

The Faint Particle Trigger (FPT) was developed for the IceCube Neutrino Observatory to enhance the detection efficiency for faint signatures, produced by free Fractionally Charged Particles (FCP) predicted in several Standard Model (SM)…

Instrumentation and Methods for Astrophysics · Physics 2024-11-04 Timo Stuerwald

Large liquid argon Time Projection Chambers have been adopted for the DUNE experiment's far detector, which will be composed of four 17 kton detectors situated 1.5 km underground at the Sanford Underground Research Facility. This represents…

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