Mariana Shopova
Bulgarian Academy of Sciences
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Publication
Featured researches published by Mariana Shopova.
Journal of Instrumentation | 2013
M. Tytgat; A. Marinov; P. Verwilligen; N. Zaganidis; A. Aleksandrov; V. Genchev; P. Iaydjiev; M. Rodozov; Mariana Shopova; G. Sultanov; Y. Assran; M. Abbrescia; C. Calabria; A. Colaleo; G. Iaselli; F. Loddo; M. Maggi; G. Pugliese; L. Benussi; S. Bianco; M. Caponero; S. Colafranceschi; F. Felli; D. Piccolo; G. Saviano; C. Carrillo; U. Berzano; M. Gabusi; P. Vitulo; M. Kang
The CMS muon system includes in both the barrel and endcap region Resistive Plate Chambers (RPC). They mainly serve as trigger detectors and also improve the reconstruction of muon parameters. Over the years, the instantaneous luminosity of the Large Hadron Collider gradually increases. During the LHC Phase 1 ( ~ first 10 years of operation) an ultimate luminosity is expected above its design value of 1034 cm−2s−1 at 14 TeV. To prepare the machine and also the experiments for this, two long shutdown periods are scheduled for 2013-2014 and 2018-2019. The CMS Collaboration is planning several detector upgrades during these long shutdowns. In particular, the muon detection system should be able to maintain a low-pT threshold for an efficient Level-1 Muon Trigger at high particle rates. One of the measures to ensure this, is to extend the present RPC system with the addition of a 4th layer in both endcap regions. During the first long shutdown, these two new stations will be equipped in the region |η| < 1.6 with 144 High Pressure Laminate (HPL) double-layer RPCs operating in avalanche mode, with a similar design as the existing CMS endcap chambers. Here, we present the upgrade plans for the CMS RPC system for the fist long shutdown, including trigger simulation studies for the extended system, and details on the new HPL production, the chamber assembly and the quality control procedures.
Journal of Instrumentation | 2013
S. Costantini; K. Beernaert; A. Cimmino; G. Garcia; J. Lellouch; A. Marinov; A. Ocampo; N. Strobbe; F. Thyssen; M. Tytgat; P. Verwilligen; E. Yazgan; N. Zaganidis; A. Dimitrov; R. Hadjiiska; L. Litov; B. Pavlov; P. Petkov; A. Aleksandrov; V. Genchev; P. Iaydjiev; M. Rodozov; Mariana Shopova; G. Sultanov; Y. Ban; J. Cai; Y. Ge; Q. Li; S. J. Qian; Z. Xue
The Resistive Plate Chambers (RPCs) are employed in the CMS experiment at the LHC as dedicated trigger system both in the barrel and in the endcap. This note presents results of the RPC detector uniformity and stability during the 2011 data taking period, and preliminary results obtained with 2012 data. The detector uniformity has been ensured with a dedicated High Voltage scan with LHC collisions, in order to determine the optimal operating working voltage of each individual RPC chamber installed in CMS. Emphasis is given on the procedures and results of the High Voltage calibration. Moreover, an increased detector stability has been obtained by automatically taking into account temperature and atmospheric pressure variations in the CMS cavern.
Journal of Instrumentation | 2012
S. Colafranceschi; L. Benussi; S. Bianco; L. Passamonti; D. Piccolo; D. Pierluigi; Antonio Russo; G. Saviano; Cristian Vendittozzi; M. Abbrescia; A. Aleksandrov; U. Berzano; C. Calabria; C. Carrillo; A. Colaleo; V. Genchev; P. Iaydjiev; M. Kang; K. S. Lee; F. Loddo; S. K. Park; G. Pugliese; M. Maggi; S. Shin; M. Rodozov; Mariana Shopova; G. Sultanov; P. Verwillingen
The Gas Gain Monitoring (GGM) system of the Resistive Plate Chamber (RPC) muon detector in the Compact Muon Solenoid (CMS) experiment provides fast and accurate determination of the stability in the working point conditions due to gas mixture changes in the closed loop recirculation system. In 2011 the GGM began to operate using a feedback algorithm to control the applied voltage, in order to keep the GGM response insensitive to environmental temperature and atmospheric pressure variations. Recent results are presented on the feedback method used and on alternative algorithms.
Journal of Instrumentation | 2012
S. K. Park; S. Choi; B. Hong; Y Gun Jeng; M. Kang; K. S. Lee; K. S. Sim; A Colaleo; G Pugliese; F Loddo; C Calabria; M Maggi; P. Verwillingen; U Berzano; C Carrillo; A. Aleksandrov; V. Genchev; P. Iaydjiev; M. Rodozov; Mariana Shopova; G. Sultanov
The CMS experiment will install a RE4 layer of 144 new Resistive Plate Chambers (RPCs) on the existing york YE3 at both endcap regions to trigger high momentum muons from the proton-proton interaction. In this paper, we present the detailed procedures used in the production of new RPC gas gaps adopted in the CMS upgrade. Quality assurance is enforced as ways to maintain the same quality of RPC gas gaps as the existing 432 endcap RPC chambers that have been operational since the beginning of the LHC operation.
Journal of Instrumentation | 2012
K. S. Lee; A. Aleksandrov; U. Berzano; C. Calabria; C. Carrillo; A. Colaleo; V. Genchev; P. Iaydjiev; Y G Jeng; M. Kang; F. Loddo; M. Maggi; S. K. Park; G. Pugliese; M. Rodozov; S. Shin; Mariana Shopova; K. S. Sim; G. Sultanov; P. Verwilligen
In this paper, we report a systematic study of multigap Resistive Plate Chambers (RPCs) for high-η triggers in CMS. Prototype RPC modules with four- and six-gap structures have been constructed with phenolic high-pressure-laminated (HPL) plates and tested with cosmic muons and gamma rays irradiated from a 200-mCi 137Cs source. The detector characteristics of the prototype multigap RPCs were compared with those of the double-gap RPCs currently used in the CMS experiment at LHC. The mean values for detector charges of cosmic-muon signals drawn in the four- and six-gap RPCs for the efficiency values in the middle of the plateau were about 1.5 and 0.9 pC, respectively, when digitized with charge thresholds of 150 and 100 fC, respectively. They were respectively about one third and one fifth of that drawn in the current CMS double-gap RPC with a charge threshold of 200 fC. We concluded from the current R&D that use of the current phenolic-HPL multigap RPCs is advantageous to the high-η triggers in CMS in virtue of the smaller detector pulses.
Journal of Instrumentation | 2016
M.I. Pedraza-Morales; Shah; Mariana Shopova
The muon spectrometer of the CMS (Compact Muon Solenoid) experiment at the Large Hadron Collider (LHC) is equipped with a redundant system made of Resistive Plate Chambers (RPCs) and Drift Tube (DT) chambers in the barrel, RPC and Cathode Strip Chambers (CSCs) in the endcap region. In this paper, the first results of the performance of the RPC system during 2015 with the LHC running at 13 TeV is presented. The stability of the RPC performance, in terms of efficiency, cluster size and noise, is reported.
Journal of Instrumentation | 2013
R. Hadjiiska; L. Litov; B. Pavlov; P. Petkov; A. Dimitrov; K. Beernaert; A. Cimmino; S. Costantini; G. Garcia; J. Lellouch; A. Marinov; A. Ocampo; N. Strobbe; F. Thyssen; M. Tytgat; P. Verwilligen; E. Yazgan; N. Zaganidis; A. Aleksandrov; V. Genchev; P. Iaydjiev; M. Rodozov; Mariana Shopova; G. Sultanov; Y. Ban; J. Cai; Z. Xue; Y. Ge; Q. Li; S. J. Qian
The Resistive Plate Chamber (RPC) muon subsystem contributes significantly to the formation of the trigger decision and reconstruction of the muon trajectory parameters. Simulation of the RPC response is a crucial part of the entire CMS Monte Carlo software and directly influences the final physical results. An algorithm based on the parametrization of RPC efficiency, noise, cluster size and timing for every strip has been developed. Experimental data obtained from cosmic and proton-proton collisions at ?s = 7 TeV have been used for determination of the parameters. A dedicated validation procedure has been developed. A good agreement between the simulated and experimental data has been achieved.
Journal of Instrumentation | 2013
P. Paolucci; R. Hadjiiska; L. Litov; B. Pavlov; P. Petkov; A. Dimitrov; K. Beernaert; A. Cimmino; S. Costantini; G. Guillaume; J. Lellouch; A. Marinov; A. Ocampo; N. Strobbe; F. Thyssen; M. Tytgat; P. Verwilligen; E. Yazgan; N. Zaganidis; A. Aleksandrov; V. Genchev; P. Iaydjiev; M. Rodozov; Mariana Shopova; G. Sultanov; Y. Ban; J. Cai; Z. Xue; Y. Ge; Q. Li
arXiv: Instrumentation and Detectors | 2018
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
arXiv: Instrumentation and Detectors | 2016
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