Cargando…
C2GT: intercepting CERN neutrinos to Gran Sasso in the Gulf of Taranto to measure $\theta_13$
Today's greatest challenge in accelerator-based neutrino physics is to measure the mixing angle \thonethree\ which is known to be much smaller than the solar mixing angle \thonetwo\ and the atmospheric mixing angle \thtwothree . A non-zero value of the angle \thonethree\ is a prerequisite for o...
Autores principales: | , , , , , , , , , , , , , , , , , , , , , , |
---|---|
Lenguaje: | eng |
Publicado: |
2006
|
Materias: | |
Acceso en línea: | https://dx.doi.org/10.1140/epjc/s10052-006-0193-3 http://cds.cern.ch/record/940418 |
_version_ | 1780909765934710784 |
---|---|
author | Ball, A E Braem, André Camilleri, L L Catinaccio, A Chelkov, G A Dydak, F Elagin, A Frandsen, Poul Kjaer Gostkin, M I Grant, A Guskov, A Joram, C Krumshtein, Z Müller, H Postema, H Price, M Rovelli, T Schinzel, D Séguinot, Jacques Valenti, G Voss, R Wotschack, J Zhemchugov, A S |
author_facet | Ball, A E Braem, André Camilleri, L L Catinaccio, A Chelkov, G A Dydak, F Elagin, A Frandsen, Poul Kjaer Gostkin, M I Grant, A Guskov, A Joram, C Krumshtein, Z Müller, H Postema, H Price, M Rovelli, T Schinzel, D Séguinot, Jacques Valenti, G Voss, R Wotschack, J Zhemchugov, A S |
author_sort | Ball, A E |
collection | CERN |
description | Today's greatest challenge in accelerator-based neutrino physics is to measure the mixing angle \thonethree\ which is known to be much smaller than the solar mixing angle \thonetwo\ and the atmospheric mixing angle \thtwothree . A non-zero value of the angle \thonethree\ is a prerequisite for observing CP violation in neutrino mixing. In this paper, we discuss a deep-sea neutrino experiment with 1.5~Mt fiducial target mass in the Gulf of Taranto with the prime objective of measuring \thonethree. The detector is exposed to the CERN neutrino beam to Gran Sasso in off-axis geometry. Monochromatic muon-neutrinos of $\approx 800$~MeV energy are the dominant beam component. Neutrinos are detected through quasi-elastic, charged-current reactions in sea water; electrons and muons are detected in a large-surface, ring-imaging Cherenkov detector. The profile of the seabed in the Gulf of Taranto allows for a moveable experiment at variable distances from CERN, starting at 1100 km. From the oscillatory pattern of the disappearance of muon-neutrinos, the experiment will measure \sthtwothree\ and especially \dmtwothree\ with high precision. The appearance of electron-neutrinos will be observed with a sensitivity to $P(\numu \rightarrow \nue$) as small as 0.0035 (90\% CL) and $\sin^2\thonethree$ as small as 0.0019 (90\% CL; for a CP phase angle $\delta = 0^\circ$ and for normal neutrino mass hierarchy). |
id | cern-940418 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2006 |
record_format | invenio |
spelling | cern-9404182019-09-30T06:29:59Zdoi:10.1140/epjc/s10052-006-0193-3http://cds.cern.ch/record/940418engBall, A EBraem, AndréCamilleri, L LCatinaccio, AChelkov, G ADydak, FElagin, AFrandsen, Poul KjaerGostkin, M IGrant, AGuskov, AJoram, CKrumshtein, ZMüller, HPostema, HPrice, MRovelli, TSchinzel, DSéguinot, JacquesValenti, GVoss, RWotschack, JZhemchugov, A SC2GT: intercepting CERN neutrinos to Gran Sasso in the Gulf of Taranto to measure $\theta_13$Particle Physics - ExperimentToday's greatest challenge in accelerator-based neutrino physics is to measure the mixing angle \thonethree\ which is known to be much smaller than the solar mixing angle \thonetwo\ and the atmospheric mixing angle \thtwothree . A non-zero value of the angle \thonethree\ is a prerequisite for observing CP violation in neutrino mixing. In this paper, we discuss a deep-sea neutrino experiment with 1.5~Mt fiducial target mass in the Gulf of Taranto with the prime objective of measuring \thonethree. The detector is exposed to the CERN neutrino beam to Gran Sasso in off-axis geometry. Monochromatic muon-neutrinos of $\approx 800$~MeV energy are the dominant beam component. Neutrinos are detected through quasi-elastic, charged-current reactions in sea water; electrons and muons are detected in a large-surface, ring-imaging Cherenkov detector. The profile of the seabed in the Gulf of Taranto allows for a moveable experiment at variable distances from CERN, starting at 1100 km. From the oscillatory pattern of the disappearance of muon-neutrinos, the experiment will measure \sthtwothree\ and especially \dmtwothree\ with high precision. The appearance of electron-neutrinos will be observed with a sensitivity to $P(\numu \rightarrow \nue$) as small as 0.0035 (90\% CL) and $\sin^2\thonethree$ as small as 0.0019 (90\% CL; for a CP phase angle $\delta = 0^\circ$ and for normal neutrino mass hierarchy).CERN-PH-EP-2006-002oai:cds.cern.ch:9404182006-03-02 |
spellingShingle | Particle Physics - Experiment Ball, A E Braem, André Camilleri, L L Catinaccio, A Chelkov, G A Dydak, F Elagin, A Frandsen, Poul Kjaer Gostkin, M I Grant, A Guskov, A Joram, C Krumshtein, Z Müller, H Postema, H Price, M Rovelli, T Schinzel, D Séguinot, Jacques Valenti, G Voss, R Wotschack, J Zhemchugov, A S C2GT: intercepting CERN neutrinos to Gran Sasso in the Gulf of Taranto to measure $\theta_13$ |
title | C2GT: intercepting CERN neutrinos to Gran Sasso in the Gulf of Taranto to measure $\theta_13$ |
title_full | C2GT: intercepting CERN neutrinos to Gran Sasso in the Gulf of Taranto to measure $\theta_13$ |
title_fullStr | C2GT: intercepting CERN neutrinos to Gran Sasso in the Gulf of Taranto to measure $\theta_13$ |
title_full_unstemmed | C2GT: intercepting CERN neutrinos to Gran Sasso in the Gulf of Taranto to measure $\theta_13$ |
title_short | C2GT: intercepting CERN neutrinos to Gran Sasso in the Gulf of Taranto to measure $\theta_13$ |
title_sort | c2gt: intercepting cern neutrinos to gran sasso in the gulf of taranto to measure $\theta_13$ |
topic | Particle Physics - Experiment |
url | https://dx.doi.org/10.1140/epjc/s10052-006-0193-3 http://cds.cern.ch/record/940418 |
work_keys_str_mv | AT ballae c2gtinterceptingcernneutrinostogransassointhegulfoftarantotomeasuretheta13 AT braemandre c2gtinterceptingcernneutrinostogransassointhegulfoftarantotomeasuretheta13 AT camillerill c2gtinterceptingcernneutrinostogransassointhegulfoftarantotomeasuretheta13 AT catinaccioa c2gtinterceptingcernneutrinostogransassointhegulfoftarantotomeasuretheta13 AT chelkovga c2gtinterceptingcernneutrinostogransassointhegulfoftarantotomeasuretheta13 AT dydakf c2gtinterceptingcernneutrinostogransassointhegulfoftarantotomeasuretheta13 AT elagina c2gtinterceptingcernneutrinostogransassointhegulfoftarantotomeasuretheta13 AT frandsenpoulkjaer c2gtinterceptingcernneutrinostogransassointhegulfoftarantotomeasuretheta13 AT gostkinmi c2gtinterceptingcernneutrinostogransassointhegulfoftarantotomeasuretheta13 AT granta c2gtinterceptingcernneutrinostogransassointhegulfoftarantotomeasuretheta13 AT guskova c2gtinterceptingcernneutrinostogransassointhegulfoftarantotomeasuretheta13 AT joramc c2gtinterceptingcernneutrinostogransassointhegulfoftarantotomeasuretheta13 AT krumshteinz c2gtinterceptingcernneutrinostogransassointhegulfoftarantotomeasuretheta13 AT mullerh c2gtinterceptingcernneutrinostogransassointhegulfoftarantotomeasuretheta13 AT postemah c2gtinterceptingcernneutrinostogransassointhegulfoftarantotomeasuretheta13 AT pricem c2gtinterceptingcernneutrinostogransassointhegulfoftarantotomeasuretheta13 AT rovellit c2gtinterceptingcernneutrinostogransassointhegulfoftarantotomeasuretheta13 AT schinzeld c2gtinterceptingcernneutrinostogransassointhegulfoftarantotomeasuretheta13 AT seguinotjacques c2gtinterceptingcernneutrinostogransassointhegulfoftarantotomeasuretheta13 AT valentig c2gtinterceptingcernneutrinostogransassointhegulfoftarantotomeasuretheta13 AT vossr c2gtinterceptingcernneutrinostogransassointhegulfoftarantotomeasuretheta13 AT wotschackj c2gtinterceptingcernneutrinostogransassointhegulfoftarantotomeasuretheta13 AT zhemchugovas c2gtinterceptingcernneutrinostogransassointhegulfoftarantotomeasuretheta13 |