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Featured researches published by Sungwoong Cho.


ORGANIZED BY THE HELLENIC PHYSICAL SOCIETY WITH THE COOPERATION OF THE PHYSICS DEPARTMENTS OF GREEK UNIVERSITIES: 7th International Conference of the Balkan Physical Union | 2010

THE CMS RPC SYSTEM OVERVIEW

N. Darmenov; V. Genchev; P. Iaydjiev; S. Stoykova; G. Sultanov; R. Trayanov; A. Dimitrov; L. Litov; B. Pavlov; P. Petkov; A. Marinov; F. Thyssen; M. Tytgat; P. Verwillingen; N. Zaganidis; S. Akimenko; A. H. Ball; I. Crotty; R. Guida; Archana Sharma; W. Van Doninck; M. Abbrescia; G. Iaselli; M. Maggi; B. Marangelli; S. Nuzzo; G. Pugliese; F. Romano; G. Roselli; R. Trentadue

The Muon System of the CMS experiment at CERN employees three different detector technologies—Drift Tube Chambers (DT) in the barrel part, Cathode Strip Chambers (CSC) in the endcaps and Resistive Plate Chambers (RPC) both in the barrel and the endcaps. TDs and CSCs serve as precise muon trajectory measurement devices. The RPCs are responsible for the bunch crossing identification and for a fast muon transverse momentum measurement. The total number of RPCs is 480 in the barrel and 756 in the endcaps, covering an area of about 3500 square meters. A brief overview of the system will be presented as well as some recent results about the system stability and performance.


Journal of Instrumentation | 2016

Radiation tests of real-sized prototype RPCs for the Phase-2 Upgrade of the CMS Muon System

K. S. Lee; Sungwoong Cho; S. Choi; B. Hong; Y. Go; M. Kang; Jaehoon Lim; Sue Kyung Park; A. Cimmino; S. Crucy; A. Fagot; M. Gul; Aao Rios; M. Tytgat; N. Zaganidis; S. Aly; Y. Assran; A. Radi; A. Sayed; G. Singh; M. Abbrescia; G. Iaselli; M. Maggi; G. Pugliese; P. Verwilligen; W. Van Doninck; S. Colafranceschi; Archana Sharma; L. Benussi; S. Bianco

We report on a systematic study of double-gap and four-gap phenolic resistive plate chambers (RPCs) for future high-{\eta} RPC triggers in the CMS. In the present study, we constructed real-sized double-gap and four-gap RPCs with gap thicknesses of 1.6 and 0.8 mm, respectively, with 2-mm-thick phenolic high-pressure-laminated (HPL) plates. We examined the prototype RPCs for cosmic rays and 100 GeV muons provided by the SPS H4 beam line at CERN. We applied maximum gamma rates of 1.5 kHz cm-2 provided by 137Cs sources at Korea University and the GIF++ irradiation facility installed at the SPS H4 beam line to examine the rate capabilities of the prototype RPCs. In contrast to the case of the four-gap RPCs, we found the relatively high threshold was conducive to effectively suppressing the rapid increase of strip cluster sizes of muon hits with high voltage, especially when measuring the narrow-pitch strips. The gamma-induced currents drawn in the four-gap RPC were about one-fourth of those drawn in the double-gap RPC. The rate capabilities of both RPC types, proven through the present testing using gamma-ray sources, far exceeded the maximum rate expected in the new high-{\eta} endcap RPCs planned for future phase-II LHC runs.We report on a systematic study of double-gap and four-gap phenolic resistive plate chambers (RPCs) for the Phase-2 upgrade of the CMS muon system at high eta. In the present study, we constructed real-sized double-gap and four-gap RPCs with gap thicknesses of 1.6 and 0.8 mm, respectively, with 2-mm-thick phenolic high-pressure-laminated (HPL) plates. We examined the prototype RPCs with cosmic rays and with 100-GeV muons provided by the SPS H4 beam line at CERN. To examine the rate capability of the prototype RPCs both at Korea University and at the CERN GIF++ facility, the chambers were irradiated with Cs-137 sources providing maximum gamma rates of about 1.5 kHz cm(-2). For the 1.6-mm-thick double-gap RPCs, we found the relatively high threshold on the produced detector charge was conducive to effectively suppressing the rapid increase of strip cluster sizes of muon hits with high voltage, especially when measuring the narrow-pitch strips. The gamma-induced currents drawn in the four-gap RPC were about one-fourth of those drawn in the double-gap RPC. The rate capabilities of both RPC types, proven through the present testing using gamma-ray sources, far exceeded the maximum rate expected in the new high-eta endcap RPCs planned for future phase-II runs of the Large Hadron Collider (LHC).


Journal of Instrumentation | 2016

R&D towards the CMS RPC Phase-2 upgrade

A. Fagot; A. Cimmino; S. Crucy; M. Gul; Aao Rios; M. Tytgat; N. Zaganidis; S. Aly; Y. Assran; A. Radi; A. Sayed; G. Singh; M. Abbrescia; G. Iaselli; M. Maggi; G. Pugliese; P. Verwilligen; W. Van Doninck; S. Colafranceschi; Archana Sharma; L. Benussi; S. Bianco; D. Piccolo; F. Primavera; V. Bhatnagar; R. Kumari; A. Mehta; J. B. Singh; A. Ahmad; W. Ahmed

The high pseudo-rapidity region of the CMS muon system is covered by Cathode Strip Chambers (CSC) only and lacks redundant coverage despite the fact that it is a challenging region for muons in terms of backgrounds and momentum resolution. In order to maintain good efficiency for the muon trigger in this region additional RPCs are planned to be installed in the two outermost stations at low angle named RE3/1 and RE4/1. These stations will use RPCs with finer granularity and good timing resolution to mitigate background effects and to increase the redundancy of the system.


Journal of Instrumentation | 2016

Detector control system and efficiency performance for CMS RPC at GIF

M. Gul; A. Braghieri; A. Magnani; I. Crotty; A. Dimitrov; J. Vaitkus; P. Vitulo; A. Fagot; F. Thyssen; C. Avila; Y. Assran; G. Pugliese; S. Buontempo; N. Zaganidis; S. Crucy; G. Lanza; G. Singh; J. B. Singh; P. Petkov; S. Muhammad; M. I. Asghar; K. S. Lee; C U Estrada; J. Goh; S. Aly; I. Bagaturia; L. Lista; Min Suk Kim; C. Riccardi; D. Kim

In the framework of the High Luminosity LHC upgrade program, the CMS muon group built several different RPC prototypes that are now under test at the new CERN Gamma Irradiation Facility (GIF++). A dedicated Detector Control System (DCS) has been developed using the WinCC-OA tool to control and monitor these prototype detectors and to store the measured parameters data. Preliminary efficiency studies that set the base performance measurements of CMS RPC for starting aging studies are also presented.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2012

Test of a four-gap resistive plate chamber with cosmic muons and high-rate gamma rays

Soung Kyu Park; S. Shin; B. Hong; G. Jhang; M. S. Jeong; M. Jo; Sungwoong Cho; E. Joo; C. Kim; H.C. Kim; K. S. Lee; S. J. Lee; Songkyo Lee; J. K. Lim; D. H. Moon; H. H. Shim; K. S. Sim


arXiv: Instrumentation and Detectors | 2018

arXiv : The CMS RPC Detector Performance and Stability during LHC RUN-2

Shah; B. Hong; G. Pugliese; M. Gouzevitch; S. Carpinteyro Bernardino; S. Carrillo Moreno; De Araujo; Mariana Shopova; I. Pedraza; C. Combaret; P. Petkov; S. Choi; J. B. Singh; I. Bagaturia; Jaehoon Lim; T. J. Kim; A. Santoro; M. Abbrescia; E. Voevodina; Jan Eysermans; K. S. Lee; Y. Assran; L. Lista; S. Aly; Martina Ressegotti; H. R. Hoorani; I. B. Laktineh; P. Vitulo; I. Orso; N. Zaganidis


Journal of the Korean Physical Society | 2018

Study of Thin Double-Gap RPCs for the CMS Muon System

K. S. Lee; Sungwoong Cho; S. Choi; B. Hong; M. Kang; Jaehoon Lim; Youngkwon Jo; S. K. Park; K. R. Ryoo; R. Aly; S. Aly; Y. Assran; A. Mohamed; A. Mahrous; S. Constantini; M. Abbrescia; A. Gelmi; M. Maggi; G. Iaselli; G. Pugliese; A. Sharma; V. Bhatnagar; R. Gupta; Priyanka Kumari; M. Manisha; J. B. Singh; L. Benussi; S. Bianc; D. Piccolo; F. Primavera


arXiv: Instrumentation and Detectors | 2016

Performance of Resistive Plate Chambers installed during the first long shutdown of the CMS experiment

Mariana Shopova; A. Aleksandrov; R. Hadjiiska; P. Iaydjiev; G. Sultanov; M. Rodozov; S. Stoykova; Y. Assran; A. Sayed; A. Radi; S. Aly; G. Singh; M. Abbrescia; G. Iaselli; M. Maggi; G. Pugliese; P. Verwilligen; W. Van Doninck; S. Colafranceschi; A. Sharma; L. Benussi; S. Bianco; D. Piccolo; F. Primavera; A. Cimmino; S. Crucy; Alberto Andres Ocampo Rios; M. Tytgat; N. Zaganidis; M. Gul


Archive | 2015

Inclusive Production of the Xð4140Þ State in p¯ p Collisions at D0

V. M. Abazov; B. Abbott; B. S. Acharya; M. Adams; T. Adams; J. P. Agnew; G. D. Alexeev; G. Alkhazov; A. Alton; A. Askew; S. Atkins; K. Augsten; C. Avila; F. Badaud; L. Bagby; B. Baldin; D. V. Bandurin; S. Banerjee; E. Barberis; P. Baringer; J. F. Bartlett; U. Bassler; V. E. Bazterra; A. Bean; M. Begalli; L. Bellantoni; S. B. Beri; G. Bernardi; R. Bernhard; I. Bertram


Archive | 2015

Precision measurement of the top-quark mass in leptonþjets final states

V. M. Abazov; B. Abbott; B. S. Acharya; M. Adams; T. Adams; J. P. Agnew; G. D. Alexeev; G. Alkhazov; A. Alton; A. Askew; S. Atkins; K. Augsten; C. Avila; F. Badaud; L. Bagby; B. Baldin; D. V. Bandurin; S. Banerjee; E. Barberis; P. Baringer; J. F. Bartlett; U. Bassler; V. E. Bazterra; A. Bean; M. Begalli; L. Bellantoni; S. B. Beri; G. Bernardi; R. Bernhard; I. Bertram

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Y. Assran

British University in Egypt

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G. Iaselli

Instituto Politécnico Nacional

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