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Neutron-proton coincidences from Non-Mesonic Weak Decay of p-shell Lambda-hypernuclei and determination of the two-nucleon induced process

The decay of Lambda-hypernuclei without pi emission, known as Non-Mesonic Weak Decay (NMWD), gives an effective tool to investigate Delta S = 1 four-baryon interactions. It was theoretically suggested that the two-nucleon induced mechanism could play a substantial role in reproducing the observed NM...

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Detalles Bibliográficos
Autores principales: Agnello, M, Benussi, L, Bertani, M, Bhang, H C, Bonomi, G, Botta, E, Bregant, M, Bressani, T, Bufalino, S, Busso, L, Calvo, D, Camerini, P, Dalena, B, De Mori, F, D'Erasmo, G, Fabbri, F L, Feliciello, A, Filippi, A, Fiore, E M, Fujioka, H, Genova, P, Gianotti, P, Grion, N, Lucherini, V, Marcello, S, Mirfakhrai, N, Moia, F, Montagna, P, Morra, O, Nagae, T, Outa, H, Pantaleo, A, Paticchio, V, Piano, S, Rui, R, Simonetti, G, Wheadon, R, Zenoni, A, Garbarino, G
Lenguaje:eng
Publicado: 2011
Materias:
Acceso en línea:https://dx.doi.org/10.1016/j.physletb.2011.06.035
http://cds.cern.ch/record/1399729
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author Agnello, M
Benussi, L
Bertani, M
Bhang, H C
Bonomi, G
Botta, E
Bregant, M
Bressani, T
Bufalino, S
Busso, L
Calvo, D
Camerini, P
Dalena, B
De Mori, F
D'Erasmo, G
Fabbri, F L
Feliciello, A
Filippi, A
Fiore, E M
Fujioka, H
Genova, P
Gianotti, P
Grion, N
Lucherini, V
Marcello, S
Mirfakhrai, N
Moia, F
Montagna, P
Morra, O
Nagae, T
Outa, H
Pantaleo, A
Paticchio, V
Piano, S
Rui, R
Simonetti, G
Wheadon, R
Zenoni, A
Garbarino, G
author_facet Agnello, M
Benussi, L
Bertani, M
Bhang, H C
Bonomi, G
Botta, E
Bregant, M
Bressani, T
Bufalino, S
Busso, L
Calvo, D
Camerini, P
Dalena, B
De Mori, F
D'Erasmo, G
Fabbri, F L
Feliciello, A
Filippi, A
Fiore, E M
Fujioka, H
Genova, P
Gianotti, P
Grion, N
Lucherini, V
Marcello, S
Mirfakhrai, N
Moia, F
Montagna, P
Morra, O
Nagae, T
Outa, H
Pantaleo, A
Paticchio, V
Piano, S
Rui, R
Simonetti, G
Wheadon, R
Zenoni, A
Garbarino, G
author_sort Agnello, M
collection CERN
description The decay of Lambda-hypernuclei without pi emission, known as Non-Mesonic Weak Decay (NMWD), gives an effective tool to investigate Delta S = 1 four-baryon interactions. It was theoretically suggested that the two-nucleon induced mechanism could play a substantial role in reproducing the observed NMWD decay rates and nucleon spectra, but at present no direct evidence of such a mechanism has been obtained. The FINUDA experiment, exploiting the possibility to detect both charged and neutral particles coming from the hypernucleus decay, has allowed us to deduce the relative weight of the two nucleon induced decay rate to the total NMWD rate. The value of Gamma(2N)/ Gamma(NMWD) = 0.21 +/- 0.07stat (+0.03sys)(-0.02sys) has been deduced, well consistent with the previous determinations.
id cern-1399729
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2011
record_format invenio
spelling cern-13997292019-09-30T06:29:59Zdoi:10.1016/j.physletb.2011.06.035http://cds.cern.ch/record/1399729engAgnello, MBenussi, LBertani, MBhang, H CBonomi, GBotta, EBregant, MBressani, TBufalino, SBusso, LCalvo, DCamerini, PDalena, BDe Mori, FD'Erasmo, GFabbri, F LFeliciello, AFilippi, AFiore, E MFujioka, HGenova, PGianotti, PGrion, NLucherini, VMarcello, SMirfakhrai, NMoia, FMontagna, PMorra, ONagae, TOuta, HPantaleo, APaticchio, VPiano, SRui, RSimonetti, GWheadon, RZenoni, AGarbarino, GNeutron-proton coincidences from Non-Mesonic Weak Decay of p-shell Lambda-hypernuclei and determination of the two-nucleon induced processNuclear Physics - ExperimentThe decay of Lambda-hypernuclei without pi emission, known as Non-Mesonic Weak Decay (NMWD), gives an effective tool to investigate Delta S = 1 four-baryon interactions. It was theoretically suggested that the two-nucleon induced mechanism could play a substantial role in reproducing the observed NMWD decay rates and nucleon spectra, but at present no direct evidence of such a mechanism has been obtained. The FINUDA experiment, exploiting the possibility to detect both charged and neutral particles coming from the hypernucleus decay, has allowed us to deduce the relative weight of the two nucleon induced decay rate to the total NMWD rate. The value of Gamma(2N)/ Gamma(NMWD) = 0.21 +/- 0.07stat (+0.03sys)(-0.02sys) has been deduced, well consistent with the previous determinations.oai:cds.cern.ch:13997292011
spellingShingle Nuclear Physics - Experiment
Agnello, M
Benussi, L
Bertani, M
Bhang, H C
Bonomi, G
Botta, E
Bregant, M
Bressani, T
Bufalino, S
Busso, L
Calvo, D
Camerini, P
Dalena, B
De Mori, F
D'Erasmo, G
Fabbri, F L
Feliciello, A
Filippi, A
Fiore, E M
Fujioka, H
Genova, P
Gianotti, P
Grion, N
Lucherini, V
Marcello, S
Mirfakhrai, N
Moia, F
Montagna, P
Morra, O
Nagae, T
Outa, H
Pantaleo, A
Paticchio, V
Piano, S
Rui, R
Simonetti, G
Wheadon, R
Zenoni, A
Garbarino, G
Neutron-proton coincidences from Non-Mesonic Weak Decay of p-shell Lambda-hypernuclei and determination of the two-nucleon induced process
title Neutron-proton coincidences from Non-Mesonic Weak Decay of p-shell Lambda-hypernuclei and determination of the two-nucleon induced process
title_full Neutron-proton coincidences from Non-Mesonic Weak Decay of p-shell Lambda-hypernuclei and determination of the two-nucleon induced process
title_fullStr Neutron-proton coincidences from Non-Mesonic Weak Decay of p-shell Lambda-hypernuclei and determination of the two-nucleon induced process
title_full_unstemmed Neutron-proton coincidences from Non-Mesonic Weak Decay of p-shell Lambda-hypernuclei and determination of the two-nucleon induced process
title_short Neutron-proton coincidences from Non-Mesonic Weak Decay of p-shell Lambda-hypernuclei and determination of the two-nucleon induced process
title_sort neutron-proton coincidences from non-mesonic weak decay of p-shell lambda-hypernuclei and determination of the two-nucleon induced process
topic Nuclear Physics - Experiment
url https://dx.doi.org/10.1016/j.physletb.2011.06.035
http://cds.cern.ch/record/1399729
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