Towards the construction of the Mu2e electromagnetic calorimeter at Fermilab
Mu2e will search for the Charge Lepton Flavor Violating (CLFV) conversion of a muon into an electron in the field of a nucleus. A clean discovery signature is provided by the mono-energetic conversion electron ( E e = 104.96 MeV). If no events are observed, Mu2e will set a limit on the ratio between...
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creator | Atanov, N. Baranov, V. Borrel, L. Bloise, C. Budagov, J. Ceravolo, S. Cervelli, F. Colao, F. Cordelli, M. Corradi, G. Davydov, Y. I. Di Falco, S. Diociaiuti, E. Donati, S. Donghia, R. Echenard, B. Ferrari, C. Gioiosa, A. Giovannella, S. Giusti, V. Glagolev, V. Grancagnolo, F. Hampai, D. Happacher, F. Hitlin, D. Lin, D. Marini, A. Martini, M. Middleton, S. Miscetti, S. Morescalchi, L. Pasciuto, D. Pedreschi, E. Porter, F. Raffaelli, F. Saputi, A. Sarra, I. Spinella, F. Taffara, A. Tassielli, G. F. Tereshchenko, V. Usubov, Z. Vasilyev, I. I. Zanetti, A. Zhu, R. Y. |
description | Mu2e will search for the Charge Lepton Flavor Violating (CLFV) conversion of a muon into an electron in the field of a nucleus. A clean discovery signature is provided by the mono-energetic conversion electron (
E
e
= 104.96 MeV). If no events are observed, Mu2e will set a limit on the ratio between the conversion and the nuclear capture rate below 3 × 10
−17
(at 90% C.L.). In order to confirm that the observed candidate is an electron, the calorimeter resolution requirements are to provide
E
res
< 10%,
T
res
< 500 ps for 100 MeV electrons while working in vacuum and in a high radiation environment and high magnetic field. The calorimeter is made of two annular aluminum disks, each one filled with 674 pure CsI crystals read out by SiPMs. A sophisticated mechanics and cooling system has been developed to support the crystals and cool the sensors. Radiation hard analog and fast digital electronics have been developed. In this paper the QC tests performed on the produced components and the construction status are reported, as well as the results obtained on the large size prototype with test beam data and at a cosmic ray test stand. |
doi_str_mv | 10.1088/1742-6596/2374/1/012021 |
format | Article |
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E
e
= 104.96 MeV). If no events are observed, Mu2e will set a limit on the ratio between the conversion and the nuclear capture rate below 3 × 10
−17
(at 90% C.L.). In order to confirm that the observed candidate is an electron, the calorimeter resolution requirements are to provide
E
res
< 10%,
T
res
< 500 ps for 100 MeV electrons while working in vacuum and in a high radiation environment and high magnetic field. The calorimeter is made of two annular aluminum disks, each one filled with 674 pure CsI crystals read out by SiPMs. A sophisticated mechanics and cooling system has been developed to support the crystals and cool the sensors. Radiation hard analog and fast digital electronics have been developed. In this paper the QC tests performed on the produced components and the construction status are reported, as well as the results obtained on the large size prototype with test beam data and at a cosmic ray test stand.</description><identifier>ISSN: 1742-6588</identifier><identifier>EISSN: 1742-6596</identifier><identifier>DOI: 10.1088/1742-6596/2374/1/012021</identifier><language>eng</language><publisher>Bristol: IOP Publishing</publisher><subject>Aluminum ; Conversion ; Cooling systems ; Cosmic rays ; Digital electronics ; Disks ; Electrons ; Flavor (particle physics) ; INSTRUMENTATION RELATED TO NUCLEAR SCIENCE AND TECHNOLOGY ; Leptons ; Nuclear capture ; Physics ; Radiation ; Test stands</subject><ispartof>Journal of Physics. Conference Series, 2022-11, Vol.2374 (1), p.12021</ispartof><rights>Published under licence by IOP Publishing Ltd</rights><rights>Published under licence by IOP Publishing Ltd. This work is published under http://creativecommons.org/licenses/by/3.0/ (the “License”). Notwithstanding the ProQuest Terms and Conditions, you may use this content in accordance with the terms of the License.</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><cites>FETCH-LOGICAL-c3011-8e9a4ae537c65612846c0b594fb795ced35aafb7248c1d92bd4fd2c6ed6f06b53</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://iopscience.iop.org/article/10.1088/1742-6596/2374/1/012021/pdf$$EPDF$$P50$$Giop$$Hfree_for_read</linktopdf><link.rule.ids>230,309,310,314,776,780,785,786,881,23909,23910,25118,27901,27902,38845,38867,53815,53842</link.rule.ids><backlink>$$Uhttps://www.osti.gov/servlets/purl/1915407$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Atanov, N.</creatorcontrib><creatorcontrib>Baranov, V.</creatorcontrib><creatorcontrib>Borrel, L.</creatorcontrib><creatorcontrib>Bloise, C.</creatorcontrib><creatorcontrib>Budagov, J.</creatorcontrib><creatorcontrib>Ceravolo, S.</creatorcontrib><creatorcontrib>Cervelli, F.</creatorcontrib><creatorcontrib>Colao, F.</creatorcontrib><creatorcontrib>Cordelli, M.</creatorcontrib><creatorcontrib>Corradi, G.</creatorcontrib><creatorcontrib>Davydov, Y. I.</creatorcontrib><creatorcontrib>Di Falco, S.</creatorcontrib><creatorcontrib>Diociaiuti, E.</creatorcontrib><creatorcontrib>Donati, S.</creatorcontrib><creatorcontrib>Donghia, R.</creatorcontrib><creatorcontrib>Echenard, B.</creatorcontrib><creatorcontrib>Ferrari, C.</creatorcontrib><creatorcontrib>Gioiosa, A.</creatorcontrib><creatorcontrib>Giovannella, S.</creatorcontrib><creatorcontrib>Giusti, V.</creatorcontrib><creatorcontrib>Glagolev, V.</creatorcontrib><creatorcontrib>Grancagnolo, F.</creatorcontrib><creatorcontrib>Hampai, D.</creatorcontrib><creatorcontrib>Happacher, F.</creatorcontrib><creatorcontrib>Hitlin, D.</creatorcontrib><creatorcontrib>Lin, D.</creatorcontrib><creatorcontrib>Marini, A.</creatorcontrib><creatorcontrib>Martini, M.</creatorcontrib><creatorcontrib>Middleton, S.</creatorcontrib><creatorcontrib>Miscetti, S.</creatorcontrib><creatorcontrib>Morescalchi, L.</creatorcontrib><creatorcontrib>Pasciuto, D.</creatorcontrib><creatorcontrib>Pedreschi, E.</creatorcontrib><creatorcontrib>Porter, F.</creatorcontrib><creatorcontrib>Raffaelli, F.</creatorcontrib><creatorcontrib>Saputi, A.</creatorcontrib><creatorcontrib>Sarra, I.</creatorcontrib><creatorcontrib>Spinella, F.</creatorcontrib><creatorcontrib>Taffara, A.</creatorcontrib><creatorcontrib>Tassielli, G. F.</creatorcontrib><creatorcontrib>Tereshchenko, V.</creatorcontrib><creatorcontrib>Usubov, Z.</creatorcontrib><creatorcontrib>Vasilyev, I. I.</creatorcontrib><creatorcontrib>Zanetti, A.</creatorcontrib><creatorcontrib>Zhu, R. Y.</creatorcontrib><creatorcontrib>Fermi National Accelerator Lab. (FNAL), Batavia, IL (United States)</creatorcontrib><title>Towards the construction of the Mu2e electromagnetic calorimeter at Fermilab</title><title>Journal of Physics. Conference Series</title><addtitle>J. Phys.: Conf. Ser</addtitle><description>Mu2e will search for the Charge Lepton Flavor Violating (CLFV) conversion of a muon into an electron in the field of a nucleus. A clean discovery signature is provided by the mono-energetic conversion electron (
E
e
= 104.96 MeV). If no events are observed, Mu2e will set a limit on the ratio between the conversion and the nuclear capture rate below 3 × 10
−17
(at 90% C.L.). In order to confirm that the observed candidate is an electron, the calorimeter resolution requirements are to provide
E
res
< 10%,
T
res
< 500 ps for 100 MeV electrons while working in vacuum and in a high radiation environment and high magnetic field. The calorimeter is made of two annular aluminum disks, each one filled with 674 pure CsI crystals read out by SiPMs. A sophisticated mechanics and cooling system has been developed to support the crystals and cool the sensors. Radiation hard analog and fast digital electronics have been developed. In this paper the QC tests performed on the produced components and the construction status are reported, as well as the results obtained on the large size prototype with test beam data and at a cosmic ray test stand.</description><subject>Aluminum</subject><subject>Conversion</subject><subject>Cooling systems</subject><subject>Cosmic rays</subject><subject>Digital electronics</subject><subject>Disks</subject><subject>Electrons</subject><subject>Flavor (particle physics)</subject><subject>INSTRUMENTATION RELATED TO NUCLEAR SCIENCE AND TECHNOLOGY</subject><subject>Leptons</subject><subject>Nuclear capture</subject><subject>Physics</subject><subject>Radiation</subject><subject>Test stands</subject><issn>1742-6588</issn><issn>1742-6596</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2022</creationdate><recordtype>article</recordtype><sourceid>O3W</sourceid><sourceid>BENPR</sourceid><recordid>eNqFkF1LwzAUhosoOKe_waJ3Qm2S5qO9lOH8YKLgvA5peuo6umYmKeK_N7UyEQRzk0PynJM3TxSdYnSJUZ6nWFCScFbwlGSCpjhFmCCC96LJ7mZ_V-f5YXTk3BqhLCwxiRZL865s5WK_glibznnba9-YLjb119lDTyCGFrS3ZqNeO_CNjrVqjW024MHGysdzsJumVeVxdFCr1sHJ9z6NXubXy9ltsni8uZtdLRKdIYyTHApFFbBMaM44JjnlGpWsoHUpCqahyphSoSY017gqSFnRuiKaQ8VrxEuWTaOzca5xvpFONx70KoTvQkqJC8woEgE6H6GtNW89OC_XprddyCWJoKIYovBAiZHS1jhnoZbb8DFlPyRGcvArB3NysCgHvxLL0W_ovBg7G7P9GX3_NHv-DcptVQc4-wP-74lPrYSJvg</recordid><startdate>20221101</startdate><enddate>20221101</enddate><creator>Atanov, N.</creator><creator>Baranov, V.</creator><creator>Borrel, L.</creator><creator>Bloise, C.</creator><creator>Budagov, J.</creator><creator>Ceravolo, S.</creator><creator>Cervelli, F.</creator><creator>Colao, F.</creator><creator>Cordelli, M.</creator><creator>Corradi, G.</creator><creator>Davydov, Y. I.</creator><creator>Di Falco, S.</creator><creator>Diociaiuti, E.</creator><creator>Donati, S.</creator><creator>Donghia, R.</creator><creator>Echenard, B.</creator><creator>Ferrari, C.</creator><creator>Gioiosa, A.</creator><creator>Giovannella, S.</creator><creator>Giusti, V.</creator><creator>Glagolev, V.</creator><creator>Grancagnolo, F.</creator><creator>Hampai, D.</creator><creator>Happacher, F.</creator><creator>Hitlin, D.</creator><creator>Lin, D.</creator><creator>Marini, A.</creator><creator>Martini, M.</creator><creator>Middleton, S.</creator><creator>Miscetti, S.</creator><creator>Morescalchi, L.</creator><creator>Pasciuto, D.</creator><creator>Pedreschi, E.</creator><creator>Porter, F.</creator><creator>Raffaelli, F.</creator><creator>Saputi, A.</creator><creator>Sarra, I.</creator><creator>Spinella, F.</creator><creator>Taffara, A.</creator><creator>Tassielli, G. F.</creator><creator>Tereshchenko, V.</creator><creator>Usubov, Z.</creator><creator>Vasilyev, I. 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I. ; Di Falco, S. ; Diociaiuti, E. ; Donati, S. ; Donghia, R. ; Echenard, B. ; Ferrari, C. ; Gioiosa, A. ; Giovannella, S. ; Giusti, V. ; Glagolev, V. ; Grancagnolo, F. ; Hampai, D. ; Happacher, F. ; Hitlin, D. ; Lin, D. ; Marini, A. ; Martini, M. ; Middleton, S. ; Miscetti, S. ; Morescalchi, L. ; Pasciuto, D. ; Pedreschi, E. ; Porter, F. ; Raffaelli, F. ; Saputi, A. ; Sarra, I. ; Spinella, F. ; Taffara, A. ; Tassielli, G. F. ; Tereshchenko, V. ; Usubov, Z. ; Vasilyev, I. I. ; Zanetti, A. ; Zhu, R. 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F.</au><au>Tereshchenko, V.</au><au>Usubov, Z.</au><au>Vasilyev, I. I.</au><au>Zanetti, A.</au><au>Zhu, R. Y.</au><aucorp>Fermi National Accelerator Lab. (FNAL), Batavia, IL (United States)</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Towards the construction of the Mu2e electromagnetic calorimeter at Fermilab</atitle><jtitle>Journal of Physics. Conference Series</jtitle><addtitle>J. Phys.: Conf. Ser</addtitle><date>2022-11-01</date><risdate>2022</risdate><volume>2374</volume><issue>1</issue><spage>12021</spage><pages>12021-</pages><issn>1742-6588</issn><eissn>1742-6596</eissn><abstract>Mu2e will search for the Charge Lepton Flavor Violating (CLFV) conversion of a muon into an electron in the field of a nucleus. A clean discovery signature is provided by the mono-energetic conversion electron (
E
e
= 104.96 MeV). If no events are observed, Mu2e will set a limit on the ratio between the conversion and the nuclear capture rate below 3 × 10
−17
(at 90% C.L.). In order to confirm that the observed candidate is an electron, the calorimeter resolution requirements are to provide
E
res
< 10%,
T
res
< 500 ps for 100 MeV electrons while working in vacuum and in a high radiation environment and high magnetic field. The calorimeter is made of two annular aluminum disks, each one filled with 674 pure CsI crystals read out by SiPMs. A sophisticated mechanics and cooling system has been developed to support the crystals and cool the sensors. Radiation hard analog and fast digital electronics have been developed. In this paper the QC tests performed on the produced components and the construction status are reported, as well as the results obtained on the large size prototype with test beam data and at a cosmic ray test stand.</abstract><cop>Bristol</cop><pub>IOP Publishing</pub><doi>10.1088/1742-6596/2374/1/012021</doi><tpages>5</tpages><oa>free_for_read</oa></addata></record> |
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source | IOP Publishing Free Content; EZB-FREE-00999 freely available EZB journals; IOPscience extra; Alma/SFX Local Collection; Free Full-Text Journals in Chemistry |
subjects | Aluminum Conversion Cooling systems Cosmic rays Digital electronics Disks Electrons Flavor (particle physics) INSTRUMENTATION RELATED TO NUCLEAR SCIENCE AND TECHNOLOGY Leptons Nuclear capture Physics Radiation Test stands |
title | Towards the construction of the Mu2e electromagnetic calorimeter at Fermilab |
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