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Related papers: A Compact TPC for the sPHENIX Experiment

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We present here v$_2$ of identified and inclusive charged particles measured in the PHENIX central arm detector ($|\eta| < 0.35$) with respect to the reaction plane defined at $|\eta| = 3 \sim 4$ in 200 GeV Au+Au collisions. We find that…

Nuclear Experiment · Physics 2009-11-07 ShinIchi Esumi

The PHENIX Experiment at RHIC has conducted a beam energy scan at several collision energies in order to search for signatures of the QCD critical point and the onset of deconfinement. PHENIX has conducted measurements of transverse energy…

Nuclear Experiment · Physics 2019-08-14 J. T. Mitchell

A new TDC-chip is under development for the COMPASS experiment at CERN. The ASIC, which exploits the 0.6 micrometer CMOS sea-of-gate technology, will allow high resolution time measurements with digitization of 75 ps, and an unprecedented…

High Energy Physics - Experiment · Physics 2007-05-23 G. Braun , H. Fischer , J. Franz , A. Grunemaier , F. H. Heinsius , K. Konigsmann , M. Schierloh , T. Schmidt , H. Schmitt , H. J. Urban

Time Projection Chamber (TPC) is one of the main tracking systems for many current and future collider experiments at RHIC and LHC. It has a capability to measure the space points of charged tracks for good momentum resolution as well as…

Instrumentation and Detectors · Physics 2019-12-30 K. Dehmelt , P. Garg , T. K. Hemmick , A. Milov , E. Shulga , V. Zakharov

The heavy ion physics approach to global event characterization has led us to instrument the forward region in the PHENIX experiment at RHIC. In heavy ion collisions this coverage yields a measurement of the "spectator" energy and its…

Nuclear Experiment · Physics 2008-11-26 Sebastian N. White

Time-of-flight measurement is an important advancement in PET scanners to improve image reconstruction with a lower delivered radiation dose. This article describes the monolithic ASIC for the TT-PET project, a novel idea for a…

This thesis summarizes the work of the author in two directions, both aimed at the study of quantum chromodynamics (QCD). The first topic presented is a measurement of groomed event shapes using archived data collected by the H1 experiment…

Nuclear Experiment · Physics 2024-09-12 Henry T. Klest

CLIC is a proposed linear $e^{+}e^{-}$ collider with center-of-mass energies of up to $3\,\textrm{TeV}$. Its main objectives are precise top quark and Higgs boson measurements, as well as searches for Beyond Standard Model physics. To meet…

Instrumentation and Detectors · Physics 2018-12-07 Simon Spannagel

This paper reports measurements of the transverse energy per unit pseudorapidity ($dE_{T}/d\eta$) produced in Au+Au collisions at $\sqrt{s_{NN}} = 200$ GeV, performed with the sPHENIX detector at the Relativistic Heavy Ion Collider (RHIC).…

Nuclear Experiment · Physics 2025-09-03 sPHENIX Collaboration , M. I. Abdulhamid , U. Acharya , E. R. Adams , G. Adawi , C. A. Aidala , Y. Akiba , M. Alfred , S. Ali , A. Alsayegh , S. Altaf , H. Amedi , D. M. Anderson , V. V. Andrieux , A. Angerami , N. Applegate , H. Aso , S. Aune , B. Azmoun , V. R. Bailey , D. Baranyai , S. Bathe , A. Bazilevsky , S. Bela , R. Belmont , J. Bennett , J. C. Bernauer , J. Bertaux , R. Bi , A. Bonenfant , S. Boose , C. Borchers , H. Bossi , R. Botsford , R. Boucher , A. Brahma , J. W. Bryan , D. Cacace , I. Cali , M. Chamizo-Llatas , S. B. Chauhan , A. Chen , D. Chen , J. Chen , K. Chen , K. Y. Chen , K. Y. Cheng , C. -Y. Chi , M. Chiu , J. Clement , E. W. Cline , M. Connors , E. Cook , R. Corliss , Y. Corrales Morales , E. Croft , N. d'Hose , A. Dabas , D. Dacosta , M. Daradkeh , S. J. Das , A. P. Dash , G. David , C. T. Dean , K. Dehmelt , X. Dong , A. Drees , J. M. Durham , A. Enokizono , H. Enyo , J. Escobar Cepero , R. Esha , B. Fadem , R. Feder , K. Finnelli , D. Firak , A. Francisco , J. Frantz , A. Frawley , K. Fujiki , M. Fujiwara , B. Garcia , P. Garg , G. Garmire , E. Gentry , Y. Go , C. Goblin , W. Goodman , Y. Goto , A. Grabas , O. Grachov , J. Granato , N. Grau , S. V. Greene , S. K. Grossberndt , R. Guidolini-Cecato , T. Hachiya , J. S. Haggerty , R. Hamilton , J. Hammond , D. A. Hangal , S. Hasegawa , M. Hata , W. He , X. He , T. Hemmick , A. Hodges , M. E. Hoffmann , A. Holt , B. Hong , M. Housenga , S. Howell , Y. Hu , H. Z. Huang , J. Huang , T. C. Huang , D. A. Huffman , C. Hughes , J. Hwang , T. Ichino , M. Ikemoto , D. Imagawa , H. Imai , D. Jah , J. James , H. -R. Jheng , Y. Ji , Z. Ji , H. Jiang , M. Kano , L. Kasper , T. Kato , Y. Kawashima , M. S. Khan , T. Kikuchi , J. Kim , B. Kimelman , H. T. Klest , A. G. Knospe , M. B. Knuesel , H. S. Ko , J. Kuczewski , N. Kumar , R. Kunnawalkam Elayavalli , C. M. Kuo , J. Kvapil , Y. Kwon , J. Lajoie , J. D. Lang , A. Lebedev , S. Lee , L. Legnosky , S. Li , X. Li , T. Lian , S. Liechty , S. Lim , D. Lis , M. X. Liu , W. J. Llope , D. A. Loomis , R. -S. Lu , L. Ma , W. Ma , V. Mahaut , T. Majoros , I. Mandjavidze , E. Mannel , C. Markert , T. R. Marshall , C. Martin , H. Masuda , G. Mattson , M. Mazeikis , C. McGinn , E. McLaughlin , J. Mead , Y. Mei , T. Mengel , M. Meskowitz , J. Mills , A. Milov , C. Mironov , G. Mitsuka , N. Morimoto , D. Morrison , L. W. Mwibanda , C. -J. Naïm , J. L. Nagle , I. Nakagawa , Y. Nakamura , G. Nakano , A. Narde , C. E. Nattrass , D. Neff , S. Nelson , D. Nemoto , P. A. Nieto-Marín , R. Nouicer , G. Nukazuka , E. O'Brien , G. Odyniec , S. Oh , V. A. Okorokov , A. C. Oliveira da Silva , J. D. Osborn , G. J. Ottino , Y. C. Ou , J. Ouellette , D. Padrazo , T. Pani , J. Park , A. Patton , H. Pereira Da Costa , D. V. Perepelitsa , M. Peters , S. Ping , C. Pinkenburg , R. Pisani , C. Platte , C. Pontieri , T. Protzman , M. L. Purschke , J. Putschke , R. J. Reed , L. Reeves , S. Regmi , E. Renner , D. Richford , C. Riedl , T. Rinn , C. Roland , G. Roland , A. Romero Hernandez , M. Rosati , D. Roy , A. Saed , T. Sakaguchi , H. Sako , S. Salur , J. Sandhu , M. Sarsour , S. Sato , B. Sayki , B. Schaefer , J. Schambach , R. Seidl , B. D. Seidlitz , Y. Sekiguchi , M. Shahid , D. M. Shangase , Z. Shi , C. W. Shih , K. Shiina , M. Shimomura , R. Shishikura , E. Shulga , A. Sickles , D. Silvermyr , R. A. Soltz , W. Sondheim , I. Sourikova , P. Steinberg , D. Stewart , S. Stoll , Y. Sugiyama , O. Suranyi , W. -C. Tang , S. Tarafdar , E. Thorsland , T. Todoroki , L. S. Tsai , H. Tsujibata , M. Tsuruta , J. Tutterow , E. Tuttle , B. Ujvari , E. N. Umaka , M. Vandenbroucke , J. Vasquez , J. Velkovska , V. Verkest , A. Vijayakumar , X. Wang , Y. Wang , Z. Wang , I. S. Ward , M. Watanabe , J. Webb , A. Wehe , A. Wils , V. Wolfe , C. Woody , W. Xie , Y. Yamaguchi , Z. Ye , K. Yip , Z. You , G. Young , C. -J. Yu , X. Yu , X. Yu , W. A. Zajc , V. Zakharov , J. Zhang , C. Zimmerli

Several new experimental concepts in high-energy particle physics have been proposed in recent years. The physical goals include precisely measuring the properties of particles such as Higgs, Z and W, and even looking for signs of new…

Instrumentation and Detectors · Physics 2022-08-17 Z. Y. Yuan , H. R. Qi , Y. Chang , L. W. Yu , Y. M. Cai , H. Y. Zhang , J. Zhang , Q. Ouyang , Y. L. Li , Z. Deng , H. Gong

A Hadron Blind Detector (HBD) is being developed for the PHENIX experiment at RHIC. It consists of a Cherenkov radiator operated with pure CF4 directly coupled in a windowless configuration to a triple-GEM detector element with a CsI…

The PHENIX Experiment at the Relativistic Heavy Ion Collider has performed a survey of momentum correlations ranging from 200 MeV/c to 7 GeV in $\sqrt{s_{NN}}$ = 200 GeV p+p, d+Au, Au+Au, and $\sqrt{s_{NN}}$ = 62 GeV Au+Au collisions. The…

Nuclear Experiment · Physics 2007-05-23 Jeffery T. Mitchell

Heavy quarks are an ideal probe of the quark gluon plasma created in heavy ion collisions. They are produced in the initial hard scattering and therefore experience the full evolution of the medium. PHENIX has previously measured the…

Nuclear Experiment · Physics 2019-08-13 D. McGlinchey

The physics aims at the proposed future CLIC high-energy linear $e^+ e^-$ collider pose challenging demands on the performance of the detector system. In particular the vertex and tracking detectors have to combine precision measurements…

Instrumentation and Detectors · Physics 2019-09-04 Mathieu Benoit

CLIC is a proposed linear e+e- collider designed to provide particle collisions at center-of-mass energies of up to 3 TeV. Precise measurements of the properties of the top quark and the Higgs boson, as well as searches for Beyond the…

Instrumentation and Detectors · Physics 2017-06-21 Simon Spannagel

The PHENIX experiment has measured transverse single spin asymmetry of J/$\Psi$ in polarized p+p collisions at forward rapidity at $\sqrt{s}=200$ GeV. The data were collected from year 2006 run of RHIC with average beam polarization of 56%.…

High Energy Physics - Experiment · Physics 2008-11-26 Han Liu

The Event Plane Detector (EPD) is an upgrade detector to the STAR experiment at RHIC, designed to measure the pattern of forward-going charged particles emitted in a high-energy collision between heavy nuclei. It consists of two…

The new concept of the spherical TPC aims at relatively large target masses with low threshold and background, keeping an extremely simple and robust operation. Such a device would open the way to detect the neutrino-nucleus interaction,…

Measurement of Bose-Einstein or HBT correlations of identified charged particles provide insight into the space-time structure of particle emitting sources in heavy-ion collisions. In this paper we present the latest results from the RHIC…

Nuclear Experiment · Physics 2016-10-21 Dániel Kincses

The properties of jets produced in p+p, d+Au and Au+Au collisions at sqrt{s_NN}=200 GeV are studied using the method of two particle correlations. The trigger particle is assumed to be a leading particle from a high p_T jet while the…

High Energy Physics - Experiment · Physics 2009-11-10 Jan Rak
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