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High rate, fast timing Glass RPC for the high ${\eta}$ CMS muon detectors

The HL-LHC phase is designed to increase by an order of magnitude the amount of data to be collected by the LHC experiments. To achieve this goal in a reasonable time scale the instantaneous luminosity would also increase by an order of magnitude up to $6.10^{34} cm^{-2} s^{-1}$ . The region of the...

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Detalles Bibliográficos
Autores principales: Lagarde, F., Gouzevitch, M., Laktineh, I., Buridon, V., Chen, X., Combaret, C., Eynard, A., Germani, L., Grenier, G., Mathez, H., Mirabito, L., Petrukhin, A., Steen, A., Tromeur, W., Wang, Y., Gong, A., Moreau, N., de la Taille, C., Dulucq, F., Cimmino, A., Crucy, S., Fagot, A., Gul, M., Rios, A.A.O., Tytgat, M., Zaganidis, N., Aly, S., Assran, Y., Radi, A., Sayed, A., Singh, G., Abbrescia, M., Iaselli, G., Maggi, M., Pugliese, G., Verwilligen, P., Van Doninck, W.F., Colafranceschi, S., Sharmag, A., Benussi, L., Bianco, S., Piccolo, D., Primavera, F., Bhatnagar, V., Kumari, R., Mehta, A., Singh, J., Ahmad, A., Ahmed, W., Asghar, M.I., Awan, I.M., Hoorani, R., Muhammad, S., Shahzad, H., Shah, M.A., Cho, S.W., Choi, S.Y., Hong, B., Kang, M.H., Lee, K.S., Lim, J.H., Park, S.K., Kim, M.S., Carpinteyro Bernardino, S., Pedraza, I., Uribe Estradam, C., Carrillo Moreno, S., Vazquez Valencia, F., Pant, L.M., Buontempo, S., Cavallo, N., Esposito, M., Fabozzi, F., Lanza, G., Orso, I., Lista, L., Meola, S., Merola, M., Paolucci, P., Thyssen, F., Braghieri, A., Magnani, A., Montagna, P., Riccardi, C., Salvini, P., Vai, I., Vitulo, P., Ban, Y., Qian, S.J., Choi, M., Choi, Y., Goh, J., Kim, D., Aleksandrov, A., Hadjiiska, R., Iaydjiev, P., Rodozov, M., Stoykova, S., Sultanov, G., Vutova, M., Dimitrov, A., Litov, L., Pavlov, B., Petkov, P., Bagaturia, I., Lomidze, D., Avila, C., Cabrera, A., Sanabria, J.C., Crotty, I., Vaitkus, J.
Formato: info:eu-repo/semantics/article
Lenguaje:eng
Publicado: JINST 2016
Materias:
Acceso en línea:https://dx.doi.org/10.1088/1748-0221/11/09/C09006
http://cds.cern.ch/record/2158668
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author Lagarde, F.
Gouzevitch, M.
Laktineh, I.
Buridon, V.
Chen, X.
Combaret, C.
Eynard, A.
Germani, L.
Grenier, G.
Mathez, H.
Mirabito, L.
Petrukhin, A.
Steen, A.
Tromeur, W.
Wang, Y.
Gong, A.
Moreau, N.
de la Taille, C.
Dulucq, F.
Cimmino, A.
Crucy, S.
Fagot, A.
Gul, M.
Rios, A.A.O.
Tytgat, M.
Zaganidis, N.
Aly, S.
Assran, Y.
Radi, A.
Sayed, A.
Singh, G.
Abbrescia, M.
Iaselli, G.
Maggi, M.
Pugliese, G.
Verwilligen, P.
Van Doninck, W.F.
Colafranceschi, S.
Sharmag, A.
Benussi, L.
Bianco, S.
Piccolo, D.
Primavera, F.
Bhatnagar, V.
Kumari, R.
Mehta, A.
Singh, J.
Ahmad, A.
Ahmed, W.
Asghar, M.I.
Awan, I.M.
Hoorani, R.
Muhammad, S.
Shahzad, H.
Shah, M.A.
Cho, S.W.
Choi, S.Y.
Hong, B.
Kang, M.H.
Lee, K.S.
Lim, J.H.
Park, S.K.
Kim, M.S.
Carpinteyro Bernardino, S.
Pedraza, I.
Uribe Estradam, C.
Carrillo Moreno, S.
Vazquez Valencia, F.
Pant, L.M.
Buontempo, S.
Cavallo, N.
Esposito, M.
Fabozzi, F.
Lanza, G.
Orso, I.
Lista, L.
Meola, S.
Merola, M.
Paolucci, P.
Thyssen, F.
Braghieri, A.
Magnani, A.
Montagna, P.
Riccardi, C.
Salvini, P.
Vai, I.
Vitulo, P.
Ban, Y.
Qian, S.J.
Choi, M.
Choi, Y.
Goh, J.
Kim, D.
Aleksandrov, A.
Hadjiiska, R.
Iaydjiev, P.
Rodozov, M.
Stoykova, S.
Sultanov, G.
Vutova, M.
Dimitrov, A.
Litov, L.
Pavlov, B.
Petkov, P.
Bagaturia, I.
Lomidze, D.
Avila, C.
Cabrera, A.
Sanabria, J.C.
Crotty, I.
Vaitkus, J.
author_facet Lagarde, F.
Gouzevitch, M.
Laktineh, I.
Buridon, V.
Chen, X.
Combaret, C.
Eynard, A.
Germani, L.
Grenier, G.
Mathez, H.
Mirabito, L.
Petrukhin, A.
Steen, A.
Tromeur, W.
Wang, Y.
Gong, A.
Moreau, N.
de la Taille, C.
Dulucq, F.
Cimmino, A.
Crucy, S.
Fagot, A.
Gul, M.
Rios, A.A.O.
Tytgat, M.
Zaganidis, N.
Aly, S.
Assran, Y.
Radi, A.
Sayed, A.
Singh, G.
Abbrescia, M.
Iaselli, G.
Maggi, M.
Pugliese, G.
Verwilligen, P.
Van Doninck, W.F.
Colafranceschi, S.
Sharmag, A.
Benussi, L.
Bianco, S.
Piccolo, D.
Primavera, F.
Bhatnagar, V.
Kumari, R.
Mehta, A.
Singh, J.
Ahmad, A.
Ahmed, W.
Asghar, M.I.
Awan, I.M.
Hoorani, R.
Muhammad, S.
Shahzad, H.
Shah, M.A.
Cho, S.W.
Choi, S.Y.
Hong, B.
Kang, M.H.
Lee, K.S.
Lim, J.H.
Park, S.K.
Kim, M.S.
Carpinteyro Bernardino, S.
Pedraza, I.
Uribe Estradam, C.
Carrillo Moreno, S.
Vazquez Valencia, F.
Pant, L.M.
Buontempo, S.
Cavallo, N.
Esposito, M.
Fabozzi, F.
Lanza, G.
Orso, I.
Lista, L.
Meola, S.
Merola, M.
Paolucci, P.
Thyssen, F.
Braghieri, A.
Magnani, A.
Montagna, P.
Riccardi, C.
Salvini, P.
Vai, I.
Vitulo, P.
Ban, Y.
Qian, S.J.
Choi, M.
Choi, Y.
Goh, J.
Kim, D.
Aleksandrov, A.
Hadjiiska, R.
Iaydjiev, P.
Rodozov, M.
Stoykova, S.
Sultanov, G.
Vutova, M.
Dimitrov, A.
Litov, L.
Pavlov, B.
Petkov, P.
Bagaturia, I.
Lomidze, D.
Avila, C.
Cabrera, A.
Sanabria, J.C.
Crotty, I.
Vaitkus, J.
author_sort Lagarde, F.
collection CERN
description The HL-LHC phase is designed to increase by an order of magnitude the amount of data to be collected by the LHC experiments. To achieve this goal in a reasonable time scale the instantaneous luminosity would also increase by an order of magnitude up to $6.10^{34} cm^{-2} s^{-1}$ . The region of the forward muon spectrometer ($|{\eta}| > 1.6$) is not equipped with RPC stations. The increase of the expected particles rate up to $2 kHz/cm^{2}$ (including a safety factor 3) motivates the installation of RPC chambers to guarantee redundancy with the CSC chambers already present. The actual RPC technology of CMS cannot sustain the expected background level. The new technology that will be chosen should have a high rate capability and provides a good spatial and timing resolution. A new generation of Glass-RPC (GRPC) using low-resistivity (LR) glass is proposed to equip at least the two most far away of the four high ${\eta}$ muon stations of CMS. First the design of small size prototypes and studies of their performance in high-rate particles flux is presented. Then the proposed designs for large size chambers and their fast-timing electronic readout are examined and preliminary results are provided.
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spelling cern-21586682022-08-10T12:36:23Z doi:10.1088/1748-0221/11/09/C09006 http://cds.cern.ch/record/2158668 eng Lagarde, F. Gouzevitch, M. Laktineh, I. Buridon, V. Chen, X. Combaret, C. Eynard, A. Germani, L. Grenier, G. Mathez, H. Mirabito, L. Petrukhin, A. Steen, A. Tromeur, W. Wang, Y. Gong, A. Moreau, N. de la Taille, C. Dulucq, F. Cimmino, A. Crucy, S. Fagot, A. Gul, M. Rios, A.A.O. Tytgat, M. Zaganidis, N. Aly, S. Assran, Y. Radi, A. Sayed, A. Singh, G. Abbrescia, M. Iaselli, G. Maggi, M. Pugliese, G. Verwilligen, P. Van Doninck, W.F. Colafranceschi, S. Sharmag, A. Benussi, L. Bianco, S. Piccolo, D. Primavera, F. Bhatnagar, V. Kumari, R. Mehta, A. Singh, J. Ahmad, A. Ahmed, W. Asghar, M.I. Awan, I.M. Hoorani, R. Muhammad, S. Shahzad, H. Shah, M.A. Cho, S.W. Choi, S.Y. Hong, B. Kang, M.H. Lee, K.S. Lim, J.H. Park, S.K. Kim, M.S. Carpinteyro Bernardino, S. Pedraza, I. Uribe Estradam, C. Carrillo Moreno, S. Vazquez Valencia, F. Pant, L.M. Buontempo, S. Cavallo, N. Esposito, M. Fabozzi, F. Lanza, G. Orso, I. Lista, L. Meola, S. Merola, M. Paolucci, P. Thyssen, F. Braghieri, A. Magnani, A. Montagna, P. Riccardi, C. Salvini, P. Vai, I. Vitulo, P. Ban, Y. Qian, S.J. Choi, M. Choi, Y. Goh, J. Kim, D. Aleksandrov, A. Hadjiiska, R. Iaydjiev, P. Rodozov, M. Stoykova, S. Sultanov, G. Vutova, M. Dimitrov, A. Litov, L. Pavlov, B. Petkov, P. Bagaturia, I. Lomidze, D. Avila, C. Cabrera, A. Sanabria, J.C. Crotty, I. Vaitkus, J. High rate, fast timing Glass RPC for the high ${\eta}$ CMS muon detectors Detectors and Experimental Techniques 13: Innovative gas detectors The HL-LHC phase is designed to increase by an order of magnitude the amount of data to be collected by the LHC experiments. To achieve this goal in a reasonable time scale the instantaneous luminosity would also increase by an order of magnitude up to $6.10^{34} cm^{-2} s^{-1}$ . The region of the forward muon spectrometer ($|{\eta}| > 1.6$) is not equipped with RPC stations. The increase of the expected particles rate up to $2 kHz/cm^{2}$ (including a safety factor 3) motivates the installation of RPC chambers to guarantee redundancy with the CSC chambers already present. The actual RPC technology of CMS cannot sustain the expected background level. The new technology that will be chosen should have a high rate capability and provides a good spatial and timing resolution. A new generation of Glass-RPC (GRPC) using low-resistivity (LR) glass is proposed to equip at least the two most far away of the four high ${\eta}$ muon stations of CMS. First the design of small size prototypes and studies of their performance in high-rate particles flux is presented. Then the proposed designs for large size chambers and their fast-timing electronic readout are examined and preliminary results are provided. The HL-LHC phase is designed to increase by an order of magnitude the amount of data to be collected by the LHC experiments. To achieve this goal in a reasonable time scale the instantaneous luminosity would also increase by an order of magnitude up to 6 · 10(34) cm(−)(2)s(−)(1). The region of the forward muon spectrometer (|η| > 1.6) is not equipped with RPC stations. The increase of the expected particles flux up to 2 kHz/cm(2) (including a safety factor 3) motivates the installation of RPC chambers to guarantee redundancy with the CSC chambers already present. The current CMS RPC technology cannot sustain the expected background level. The new technology that will be chosen should have a high rate capability and provide a good spatial and timing resolution. A new generation of Glass-RPC (GRPC) using low-resistivity glass is proposed to equip at least the two most far away of the four high η muon stations of CMS. First the design of small size prototypes and studies of their performance in high-rate particles flux are presented. Then the proposed designs for large size chambers and their fast-timing electronic readout are examined and preliminary results are provided. The HL-LHC phase is designed to increase by an order of magnitude the amount of data to be collected by the LHC experiments. To achieve this goal in a reasonable time scale the instantaneous luminosity would also increase by an order of magnitude up to $6.10^{34} cm^{-2} s^{-1}$ . The region of the forward muon spectrometer ($|{\eta}| > 1.6$) is not equipped with RPC stations. The increase of the expected particles rate up to $2 kHz/cm^{2}$ (including a safety factor 3) motivates the installation of RPC chambers to guarantee redundancy with the CSC chambers already present. The actual RPC technology of CMS cannot sustain the expected background level. The new technology that will be chosen should have a high rate capability and provides a good spatial and timing resolution. A new generation of Glass-RPC (GRPC) using low-resistivity (LR) glass is proposed to equip at least the two most far away of the four high ${\eta}$ muon stations of CMS. First the design of small size prototypes and studies of their performance in high-rate particles flux is presented. Then the proposed designs for large size chambers and their fast-timing electronic readout are examined and preliminary results are provided. info:eu-repo/grantAgreement/EC/FP7/654168 info:eu-repo/semantics/openAccess Education Level info:eu-repo/semantics/article http://cds.cern.ch/record/2158668 JINST JINST, (2016) pp. C09006 2016-02-22
spellingShingle Detectors and Experimental Techniques
13: Innovative gas detectors
Lagarde, F.
Gouzevitch, M.
Laktineh, I.
Buridon, V.
Chen, X.
Combaret, C.
Eynard, A.
Germani, L.
Grenier, G.
Mathez, H.
Mirabito, L.
Petrukhin, A.
Steen, A.
Tromeur, W.
Wang, Y.
Gong, A.
Moreau, N.
de la Taille, C.
Dulucq, F.
Cimmino, A.
Crucy, S.
Fagot, A.
Gul, M.
Rios, A.A.O.
Tytgat, M.
Zaganidis, N.
Aly, S.
Assran, Y.
Radi, A.
Sayed, A.
Singh, G.
Abbrescia, M.
Iaselli, G.
Maggi, M.
Pugliese, G.
Verwilligen, P.
Van Doninck, W.F.
Colafranceschi, S.
Sharmag, A.
Benussi, L.
Bianco, S.
Piccolo, D.
Primavera, F.
Bhatnagar, V.
Kumari, R.
Mehta, A.
Singh, J.
Ahmad, A.
Ahmed, W.
Asghar, M.I.
Awan, I.M.
Hoorani, R.
Muhammad, S.
Shahzad, H.
Shah, M.A.
Cho, S.W.
Choi, S.Y.
Hong, B.
Kang, M.H.
Lee, K.S.
Lim, J.H.
Park, S.K.
Kim, M.S.
Carpinteyro Bernardino, S.
Pedraza, I.
Uribe Estradam, C.
Carrillo Moreno, S.
Vazquez Valencia, F.
Pant, L.M.
Buontempo, S.
Cavallo, N.
Esposito, M.
Fabozzi, F.
Lanza, G.
Orso, I.
Lista, L.
Meola, S.
Merola, M.
Paolucci, P.
Thyssen, F.
Braghieri, A.
Magnani, A.
Montagna, P.
Riccardi, C.
Salvini, P.
Vai, I.
Vitulo, P.
Ban, Y.
Qian, S.J.
Choi, M.
Choi, Y.
Goh, J.
Kim, D.
Aleksandrov, A.
Hadjiiska, R.
Iaydjiev, P.
Rodozov, M.
Stoykova, S.
Sultanov, G.
Vutova, M.
Dimitrov, A.
Litov, L.
Pavlov, B.
Petkov, P.
Bagaturia, I.
Lomidze, D.
Avila, C.
Cabrera, A.
Sanabria, J.C.
Crotty, I.
Vaitkus, J.
High rate, fast timing Glass RPC for the high ${\eta}$ CMS muon detectors
title High rate, fast timing Glass RPC for the high ${\eta}$ CMS muon detectors
title_full High rate, fast timing Glass RPC for the high ${\eta}$ CMS muon detectors
title_fullStr High rate, fast timing Glass RPC for the high ${\eta}$ CMS muon detectors
title_full_unstemmed High rate, fast timing Glass RPC for the high ${\eta}$ CMS muon detectors
title_short High rate, fast timing Glass RPC for the high ${\eta}$ CMS muon detectors
title_sort high rate, fast timing glass rpc for the high ${\eta}$ cms muon detectors
topic Detectors and Experimental Techniques
13: Innovative gas detectors
url https://dx.doi.org/10.1088/1748-0221/11/09/C09006
http://cds.cern.ch/record/2158668
http://cds.cern.ch/record/2158668
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AT bagaturiai highratefasttimingglassrpcforthehighetacmsmuondetectors
AT lomidzed highratefasttimingglassrpcforthehighetacmsmuondetectors
AT avilac highratefasttimingglassrpcforthehighetacmsmuondetectors
AT cabreraa highratefasttimingglassrpcforthehighetacmsmuondetectors
AT sanabriajc highratefasttimingglassrpcforthehighetacmsmuondetectors
AT crottyi highratefasttimingglassrpcforthehighetacmsmuondetectors
AT vaitkusj highratefasttimingglassrpcforthehighetacmsmuondetectors