Cargando…
The charged anticounter for the NA62 experiment at CERN
The NA62 experiment at CERN aims at measuring the Branching-Ratio (BR) of the ultra-rare kaon decay K+ → π+ ν with 10% relative uncertainty, using an unseparated positive hadron beam of 75GeV/c, in order to test the Standard Model (SM) measuring the |Vtd| element of the Cabibbo-Kobayashi-Maskawa (CK...
Autores principales: | , , , , , , , , , , |
---|---|
Lenguaje: | eng |
Publicado: |
2014
|
Materias: | |
Acceso en línea: | https://dx.doi.org/10.1142/9789814603164_0060 http://cds.cern.ch/record/2025808 |
_version_ | 1780947221179531264 |
---|---|
author | Ambrosino, F Capussela, T DI Filippo, D Massarotti, P Mirra, M Napolitano, M Roscilli, L Saracino, G Corradi, G Paglia, C Tagnani, D |
author_facet | Ambrosino, F Capussela, T DI Filippo, D Massarotti, P Mirra, M Napolitano, M Roscilli, L Saracino, G Corradi, G Paglia, C Tagnani, D |
author_sort | Ambrosino, F |
collection | CERN |
description | The NA62 experiment at CERN aims at measuring the Branching-Ratio (BR) of the ultra-rare kaon decay K+ → π+ ν with 10% relative uncertainty, using an unseparated positive hadron beam of 75GeV/c, in order to test the Standard Model (SM) measuring the |Vtd| element of the Cabibbo-Kobayashi-Maskawa (CKM) flavour mixing matrix and to possibly search for physics Beyond SM. Backgrounds, which are up to 1010 times higher than the signal, will be suppressed by an accurate measurement of the momentum and direction of the K+ and the π+ and by a complex system of veto detectors. A critical background can be induced by inelastic interactions of the hadron beam with the silicon beam tracker. Pions produced in these interactions, emitted at low angle, can mimic a K decay in the fiducial region if no other track is detected. In order to suppress this background a CHarged track ANTIcounter (CHANTI), has been designed and is in construction. The detector consists of a series of six guard counters surrounding the beam and placed immediately after the Silicon tracker. Each ring is made of scintillator bars; light produced in a bar is collected by a wavelength-shifting (WLS) fiber running inside the bar. The fiber is read from one side by Hamamatsu Silicon Photo-Multiplier (SiPM); the other side of the fiber is mirrored. We describe the design and of the CHANTI and report on results obtained testing a prototype. |
id | oai-inspirehep.net-1320876 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2014 |
record_format | invenio |
spelling | oai-inspirehep.net-13208762019-09-30T06:29:59Zdoi:10.1142/9789814603164_0060http://cds.cern.ch/record/2025808engAmbrosino, FCapussela, TDI Filippo, DMassarotti, PMirra, MNapolitano, MRoscilli, LSaracino, GCorradi, GPaglia, CTagnani, DThe charged anticounter for the NA62 experiment at CERNDetectors and Experimental TechniquesThe NA62 experiment at CERN aims at measuring the Branching-Ratio (BR) of the ultra-rare kaon decay K+ → π+ ν with 10% relative uncertainty, using an unseparated positive hadron beam of 75GeV/c, in order to test the Standard Model (SM) measuring the |Vtd| element of the Cabibbo-Kobayashi-Maskawa (CKM) flavour mixing matrix and to possibly search for physics Beyond SM. Backgrounds, which are up to 1010 times higher than the signal, will be suppressed by an accurate measurement of the momentum and direction of the K+ and the π+ and by a complex system of veto detectors. A critical background can be induced by inelastic interactions of the hadron beam with the silicon beam tracker. Pions produced in these interactions, emitted at low angle, can mimic a K decay in the fiducial region if no other track is detected. In order to suppress this background a CHarged track ANTIcounter (CHANTI), has been designed and is in construction. The detector consists of a series of six guard counters surrounding the beam and placed immediately after the Silicon tracker. Each ring is made of scintillator bars; light produced in a bar is collected by a wavelength-shifting (WLS) fiber running inside the bar. The fiber is read from one side by Hamamatsu Silicon Photo-Multiplier (SiPM); the other side of the fiber is mirrored. We describe the design and of the CHANTI and report on results obtained testing a prototype.oai:inspirehep.net:13208762014 |
spellingShingle | Detectors and Experimental Techniques Ambrosino, F Capussela, T DI Filippo, D Massarotti, P Mirra, M Napolitano, M Roscilli, L Saracino, G Corradi, G Paglia, C Tagnani, D The charged anticounter for the NA62 experiment at CERN |
title | The charged anticounter for the NA62 experiment at CERN |
title_full | The charged anticounter for the NA62 experiment at CERN |
title_fullStr | The charged anticounter for the NA62 experiment at CERN |
title_full_unstemmed | The charged anticounter for the NA62 experiment at CERN |
title_short | The charged anticounter for the NA62 experiment at CERN |
title_sort | charged anticounter for the na62 experiment at cern |
topic | Detectors and Experimental Techniques |
url | https://dx.doi.org/10.1142/9789814603164_0060 http://cds.cern.ch/record/2025808 |
work_keys_str_mv | AT ambrosinof thechargedanticounterforthena62experimentatcern AT capusselat thechargedanticounterforthena62experimentatcern AT difilippod thechargedanticounterforthena62experimentatcern AT massarottip thechargedanticounterforthena62experimentatcern AT mirram thechargedanticounterforthena62experimentatcern AT napolitanom thechargedanticounterforthena62experimentatcern AT roscillil thechargedanticounterforthena62experimentatcern AT saracinog thechargedanticounterforthena62experimentatcern AT corradig thechargedanticounterforthena62experimentatcern AT pagliac thechargedanticounterforthena62experimentatcern AT tagnanid thechargedanticounterforthena62experimentatcern AT ambrosinof chargedanticounterforthena62experimentatcern AT capusselat chargedanticounterforthena62experimentatcern AT difilippod chargedanticounterforthena62experimentatcern AT massarottip chargedanticounterforthena62experimentatcern AT mirram chargedanticounterforthena62experimentatcern AT napolitanom chargedanticounterforthena62experimentatcern AT roscillil chargedanticounterforthena62experimentatcern AT saracinog chargedanticounterforthena62experimentatcern AT corradig chargedanticounterforthena62experimentatcern AT pagliac chargedanticounterforthena62experimentatcern AT tagnanid chargedanticounterforthena62experimentatcern |