Effects of one valence proton on seniority and angular momentum of neutrons in neutron-rich <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mmultiscripts><mml:mi>Sb</mml:mi><mml:mprescripts/><mml:mn>51</mml:mn><mml:mrow><mml:mn>122</mml:mn><mml:mo>–</mml:mo><mml:mn>131</mml:mn></mml:mrow></mml:mmultiscripts></mml:math> isotopes
S. BiswasCommissariat à l'Énergie Atomique et aux Énergies AlternativesA. LemassonLaboratoire National Henri BecquerelM. RejmundLaboratoire National Henri BecquerelA. NavinLaboratoire National Henri BecquerelY. H. KimLaboratoire National Henri BecquerelC. MichelagnoliGANIL, CEA/DRF-CNRS/IN2P3, Bd Henri Becquerel, BP 55027, F-14076 Caen Cedex 5, FranceI. StefanInstitut de Physique Nucléaire, IN2P3-CNRS, Univ. Paris Sud, Université Paris Saclay, 91406 Orsay Cedex, FranceR. BanikVariable Energy Cyclotron Centre, 1/AF Bidhan Nagar, Kolkata 700064, IndiaP. BednarczykInstitute of Nuclear Physics PAN, Kraków, PolandS. BhattacharyaVariable Energy Cyclotron Centre, 1/AF Bidhan Nagar, Kolkata 700064, IndiaS. BhattacharyyaHomi Bhabha National Institute, Training School Complex, Anushaktinagar, Mumbai-400094, IndiaE. ClémentCommissariat à l'Énergie Atomique et aux Énergies AlternativesH. L. CrawfordNuclear Science Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USAG. de FranceLaboratoire National Henri BecquerelP. FallonNuclear Science Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USAG. FrémontGrand Accélérateur National d'Ions LourdsJ. GoupilGrand Accélérateur National d'Ions LourdsB. JacquotLaboratoire National Henri BecquerelH. J. LiGANIL, CEA/DRF-CNRS/IN2P3, Bd Henri Becquerel, BP 55027, F-14076 Caen Cedex 5, FranceJ. LjungvallCSNSM, Univ. Paris-Sud, CNRS/IN2P3, Université Paris-Saclay, 91405 Orsay, FranceA. MajInstitute of Nuclear Physics PAN, Krakw, PolandLoïc MénagerGANIL, CEA/DRF-CNRS/IN2P3, Bd Henri Becquerel, BP 55027, F-14076 Caen Cedex 5, FranceV. MorelGrand Accélérateur National d'Ions LourdsR. PalitDepartment of Nuclear and Atomic Physics, Tata Institute of Fundamental Research, Mumbai 400005, IndiaR. M. Pérez-VidalInstituto de Física CorpuscularJ. RopertGANIL, CEA/DRF-CNRS/IN2P3, Bd Henri Becquerel, BP 55027, F-14076 Caen Cedex 5, FranceD. BarrientosCERN, CH-1211 Geneva 23 (Switzerland)G. BenzoniINFN, Sezione di Milano, Milano, ItalyB. BirkenbachInstitut fr Kernphysik, Universitt zu Kln, Zlpicher Str. 77, D-50937 Kln, GermanyA.J. BostonOliver Lodge Laboratory, The University of Liverpool, Liverpool, L69 7ZE, United KingdomH.C. BostonOliver Lodge Laboratory, The University of Liverpool, Liverpool, L69 7ZE, United KingdomB. CederwallOliver Lodge Laboratory, The University of Liverpool, Liverpool, L69 7ZE, United KingdomJ. ColladoDepartamento de Ingeniera Electrnica, Universitat de Valencia, Burjassot, Valencia, SpainD. M. CullenNuclear Physics Group, Schuster Laboratory, University of Manchester, Manchester, M13 9PL, United KingdomP. DésesquellesCentre National de la Recherche ScientifiqueC. Domingo‐PardoInstituto de Fsica Corpuscular, CSIC-Universitat de Valncia, E-46980 Valncia, SpainJ. DudouetUniversité de Lyon, Université Lyon-1, CNRS/IN2P3, UMR5822, IPNL, 4 Rue Enrico Fermi, F-69622 Villeurbanne Cedex, FranceJ. EberthInstitut fr Kernphysik, Universitt zu Kln, Zlpicher Str. 77, D-50937 Kln, GermanyV. GonzálezDepartamento de Ingeniería Electrónica, Universitat de Valencia, Burjassot, Valencia, SpainL. J. Harkness-BrennanOliver Lodge Laboratory, The University of Liverpool, Liverpool, L69 7ZE, United KingdomH. HessInstitut fr Kernphysik, Universitt zu Kln, Zlpicher Str. 77, D-50937 Kln, GermanyA. JungclausInstituto de Estructura de la Materia, CSIC, Madrid, E-28006 Madrid, SpainW. KortenCEA Paris-SaclayM. LabicheSTFC Daresbury Laboratory, Daresbury, Warrington, WA4 4AD, United KingdomA. LefèvreLaboratoire National Henri BecquerelR. MenegazzoINFN Sezione di Padova, I-35131 Padova, ItalyD. MengoniDipartimento di Fisica e Astronomia dell'Universit di Padova, I-35131 Padova, ItalyB. MillionINFN, Sezione di Milano, Milano, ItalyD. R. NapoliINFN, Laboratori Nazionali di Legnaro, Via Romea 4, I-35020 Legnaro, ItalyA. PulliaINFN, Sezione di Milano, Milano, ItalyB. QuintanaLaboratorio de Radiaciones Ionizantes, Universidad de Salamanca, E-37008 Salamanca, SpainD. RaletInstitut für Kernphysik, Technische Universität Darmstadt, D-64289 Darmstadt, GermanyF. RecchiaDipartimento di Fisica e Astronomia dell'Universit di Padova, I-35131 Padova, ItalyP. ReiterInstitut fr Kernphysik, Universitt zu Kln, Zlpicher Str. 77, D-50937 Kln, GermanyF. SaillantGrand Accélérateur National d'Ions LourdsM.-D. SalsacIRFU, CEA/DRF, Centre CEA de Saclay, F-91191 Gif-sur-Yvette Cedex, FranceE. SanchísDepartamento de Ingeniera Electrnica, Universitat de Valencia, Burjassot, Valencia, SpainO. StézowskiInstitute of Nuclear Physics of LyonCh. TheisenIRFU, CEA/DRF, Centre CEA de Saclay, F-91191 Gif-sur-Yvette Cedex, FranceJ. J. Valiente-DobónINFN, Laboratori Nazionali di Legnaro, Via Romea 4, I-35020 Legnaro, ItalyM. ZielińskaCEA Paris-Saclay - Etablissement de Saclay
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Background: Levels fulfilling the seniority scheme and relevant isomers are commonly observed features in semimagic nuclei; for example, in Sn isotopes (Z = 50). Seniority isomers in Sn, with dominantly pure neutron configurations, directly probe the underlying neutron-neutron () interaction. Furthermore, an addition of a valence proton particle or hole, through neutron-proton () interaction, affects the neutron seniority as well as the angular momentum.
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