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Spectroscopy of $^{46}$Ar by the $(t,p)$ two-neutron transfer reaction

States in the $N=28$ nucleus $^{46}$Ar have been studied by a two-neutron transfer reaction at REX-ISOLDE (CERN). A beam of radioactive $^{44}$ at an energy of 2.16~AMeV and a tritium loaded titanium target were used to populate $^{46}$ by the t($^{44}$,p) two-neutron transfer reaction. Protons emit...

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Detalles Bibliográficos
Autores principales: Nowak, K., Wimmer, K., Hellgartner, S., Mücher, D., Bildstein, V., Diriken, J., Elseviers, J., Gaffney, L.P., Gernhäuser, R., Iwanicki, J., Johansen, J.G., Huyse, M., Konki, J., Kröll, T., Krücken, T., Lutter, R., Orlandi, R., Pakarinen, J., Raabe, R., Reiter, P., Roger, T., Schrieder, G., Seidlitz, M., Sorlin, O., Van Duppen, P., Warr, N., De Witte, H., Zielinska, M.
Lenguaje:eng
Publicado: 2016
Materias:
Acceso en línea:https://dx.doi.org/10.1103/PhysRevC.93.044335
http://cds.cern.ch/record/2146291
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author Nowak, K.
Wimmer, K.
Hellgartner, S.
Mücher, D.
Bildstein, V.
Diriken, J.
Elseviers, J.
Gaffney, L.P.
Gernhäuser, R.
Iwanicki, J.
Johansen, J.G.
Huyse, M.
Konki, J.
Kröll, T.
Krücken, T.
Lutter, R.
Orlandi, R.
Pakarinen, J.
Raabe, R.
Reiter, P.
Roger, T.
Schrieder, G.
Seidlitz, M.
Sorlin, O.
Van Duppen, P.
Warr, N.
De Witte, H.
Zielinska, M.
author_facet Nowak, K.
Wimmer, K.
Hellgartner, S.
Mücher, D.
Bildstein, V.
Diriken, J.
Elseviers, J.
Gaffney, L.P.
Gernhäuser, R.
Iwanicki, J.
Johansen, J.G.
Huyse, M.
Konki, J.
Kröll, T.
Krücken, T.
Lutter, R.
Orlandi, R.
Pakarinen, J.
Raabe, R.
Reiter, P.
Roger, T.
Schrieder, G.
Seidlitz, M.
Sorlin, O.
Van Duppen, P.
Warr, N.
De Witte, H.
Zielinska, M.
author_sort Nowak, K.
collection CERN
description States in the $N=28$ nucleus $^{46}$Ar have been studied by a two-neutron transfer reaction at REX-ISOLDE (CERN). A beam of radioactive $^{44}$ at an energy of 2.16~AMeV and a tritium loaded titanium target were used to populate $^{46}$ by the t($^{44}$,p) two-neutron transfer reaction. Protons emitted from the target were identified in the T-REX silicon detector array. The excitation energies of states in $^{46}$ have been reconstructed from the measured angles and energies of recoil protons. Angular distributions for three final states were measured and based on the shape of the differential cross section an excited state at 3695~keV has been identified as $J^\pi = 0^+$. The angular differential cross section for the population of different states are compared to calculations using a reaction model employing both sequential and direct transfer of two neutrons. Results are compared to shell model calculations using state-of-the-art effective interactions.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2016
record_format invenio
spelling cern-21462912022-04-22T08:44:49Zdoi:10.1103/PhysRevC.93.044335http://cds.cern.ch/record/2146291engNowak, K.Wimmer, K.Hellgartner, S.Mücher, D.Bildstein, V.Diriken, J.Elseviers, J.Gaffney, L.P.Gernhäuser, R.Iwanicki, J.Johansen, J.G.Huyse, M.Konki, J.Kröll, T.Krücken, T.Lutter, R.Orlandi, R.Pakarinen, J.Raabe, R.Reiter, P.Roger, T.Schrieder, G.Seidlitz, M.Sorlin, O.Van Duppen, P.Warr, N.De Witte, H.Zielinska, M.Spectroscopy of $^{46}$Ar by the $(t,p)$ two-neutron transfer reactionNuclear Physics - ExperimentStates in the $N=28$ nucleus $^{46}$Ar have been studied by a two-neutron transfer reaction at REX-ISOLDE (CERN). A beam of radioactive $^{44}$ at an energy of 2.16~AMeV and a tritium loaded titanium target were used to populate $^{46}$ by the t($^{44}$,p) two-neutron transfer reaction. Protons emitted from the target were identified in the T-REX silicon detector array. The excitation energies of states in $^{46}$ have been reconstructed from the measured angles and energies of recoil protons. Angular distributions for three final states were measured and based on the shape of the differential cross section an excited state at 3695~keV has been identified as $J^\pi = 0^+$. The angular differential cross section for the population of different states are compared to calculations using a reaction model employing both sequential and direct transfer of two neutrons. Results are compared to shell model calculations using state-of-the-art effective interactions.States in the N=28 nucleus Ar46 have been studied by a two-neutron transfer reaction at REX-ISOLDE (CERN). A beam of radioactive Ar44 at an energy of 2.16 AMeV and a tritium-loaded titanium target were used to populate Ar46 by the H3(Ar44,p) two-neutron transfer reaction. Protons emitted from the target were identified in the T-REX silicon detector array. The excitation energies of states in Ar46 have been reconstructed from the measured angles and energies of recoil protons. Angular distributions for three final states were measured and based on the shape of the differential cross section an excited state at 3695 keV was identified as Jπ=0+. The angular differential cross section for the population of different states are compared to calculations using a reaction model employing both sequential and direct transfer of two neutrons. Results are compared to shell-model calculations using state-of-the-art effective interactions.States in the $N=28$ nucleus $^{46}$Ar have been studied by a two-neutron transfer reaction at REX-ISOLDE (CERN). A beam of radioactive $^{44}$ at an energy of 2.16~AMeV and a tritium loaded titanium target were used to populate $^{46}$ by the t($^{44}$,p) two-neutron transfer reaction. Protons emitted from the target were identified in the T-REX silicon detector array. The excitation energies of states in $^{46}$ have been reconstructed from the measured angles and energies of recoil protons. Angular distributions for three final states were measured and based on the shape of the differential cross section an excited state at 3695~keV has been identified as $J^\pi = 0^+$. The angular differential cross section for the population of different states are compared to calculations using a reaction model employing both sequential and direct transfer of two neutrons. Results are compared to shell model calculations using state-of-the-art effective interactions.arXiv:1604.04014oai:cds.cern.ch:21462912016-04-13
spellingShingle Nuclear Physics - Experiment
Nowak, K.
Wimmer, K.
Hellgartner, S.
Mücher, D.
Bildstein, V.
Diriken, J.
Elseviers, J.
Gaffney, L.P.
Gernhäuser, R.
Iwanicki, J.
Johansen, J.G.
Huyse, M.
Konki, J.
Kröll, T.
Krücken, T.
Lutter, R.
Orlandi, R.
Pakarinen, J.
Raabe, R.
Reiter, P.
Roger, T.
Schrieder, G.
Seidlitz, M.
Sorlin, O.
Van Duppen, P.
Warr, N.
De Witte, H.
Zielinska, M.
Spectroscopy of $^{46}$Ar by the $(t,p)$ two-neutron transfer reaction
title Spectroscopy of $^{46}$Ar by the $(t,p)$ two-neutron transfer reaction
title_full Spectroscopy of $^{46}$Ar by the $(t,p)$ two-neutron transfer reaction
title_fullStr Spectroscopy of $^{46}$Ar by the $(t,p)$ two-neutron transfer reaction
title_full_unstemmed Spectroscopy of $^{46}$Ar by the $(t,p)$ two-neutron transfer reaction
title_short Spectroscopy of $^{46}$Ar by the $(t,p)$ two-neutron transfer reaction
title_sort spectroscopy of $^{46}$ar by the $(t,p)$ two-neutron transfer reaction
topic Nuclear Physics - Experiment
url https://dx.doi.org/10.1103/PhysRevC.93.044335
http://cds.cern.ch/record/2146291
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