The magic nature of 132Sn explored through the single-particle states of 133Sn
Nuclear magic Atomic nuclei have a shell structure that allows for 'magic' numbers of neutrons and protons, analogous to the noble gases in atomic physics. Knowledge of the properties of single-particle states outside nuclear shell closures in exotic nuclei is important for fundamental und...
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Published in | Nature (London) Vol. 465; no. 7297; pp. 454 - 457 |
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Main Authors | , , , , , , , , , , , , , , , , , , , , , , , , |
Format | Journal Article |
Language | English |
Published |
London
Nature Publishing Group UK
01.05.2010
Nature Publishing Group |
Subjects | |
Online Access | Get full text |
ISSN | 0028-0836 1476-4687 |
DOI | 10.1038/nature09048 |
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Abstract | Nuclear magic
Atomic nuclei have a shell structure that allows for 'magic' numbers of neutrons and protons, analogous to the noble gases in atomic physics. Knowledge of the properties of single-particle states outside nuclear shell closures in exotic nuclei is important for fundamental understanding of nuclear structure and nucleosynthesis. Using a nucleon transfer technique to add single neutrons to the short-lived tin isotope
132
Sn, to create the even-shorter-lived
133
Sn, Jones
et al
. have been able to confirm the closed-shell 'doubly magic' nature of
132
Sn. Measurements of the spectrum of quantum states available to the added neutron show that the characteristics of the
133
Sn nucleus are determined almost completely by this single neutron. This finding extends the validity of the shell model to neutron-rich nuclei, and provides a benchmark for predicting the properties of nuclei even farther from stability, including those involved in neutron-capture reactions in supernovae.
Atomic nuclei have a shell structure that allows for 'magic numbers' of neutrons and protons, analogous to the noble gases in atomic physics. Knowledge of the properties of single-particle states outside nuclear shell closures in exotic nuclei is important for the fundamental understanding of nuclear structure and nucleosynthesis. Here, a nucleon-transfer technique has been used to measure the single-particle states of
133
Sn, revealing the highly magic nature of
132
Sn.
Atomic nuclei have a shell structure
1
in which nuclei with ‘magic numbers’ of neutrons and protons are analogous to the noble gases in atomic physics. Only ten nuclei with the standard magic numbers of both neutrons and protons have so far been observed. The nuclear shell model is founded on the precept that neutrons and protons can move as independent particles in orbitals with discrete quantum numbers, subject to a mean field generated by all the other nucleons. Knowledge of the properties of single-particle states outside nuclear shell closures in exotic nuclei is important
2
,
3
,
4
,
5
for a fundamental understanding of nuclear structure and nucleosynthesis (for example the r-process, which is responsible for the production of about half of the heavy elements). However, as a result of their short lifetimes, there is a paucity of knowledge about the nature of single-particle states outside exotic doubly magic nuclei. Here we measure the single-particle character of the levels in
133
Sn that lie outside the double shell closure present at the short-lived nucleus
132
Sn. We use an inverse kinematics technique that involves the transfer of a single nucleon to the nucleus. The purity of the measured single-particle states clearly illustrates the magic nature of
132
Sn. |
---|---|
AbstractList | Nuclear magic
Atomic nuclei have a shell structure that allows for 'magic' numbers of neutrons and protons, analogous to the noble gases in atomic physics. Knowledge of the properties of single-particle states outside nuclear shell closures in exotic nuclei is important for fundamental understanding of nuclear structure and nucleosynthesis. Using a nucleon transfer technique to add single neutrons to the short-lived tin isotope
132
Sn, to create the even-shorter-lived
133
Sn, Jones
et al
. have been able to confirm the closed-shell 'doubly magic' nature of
132
Sn. Measurements of the spectrum of quantum states available to the added neutron show that the characteristics of the
133
Sn nucleus are determined almost completely by this single neutron. This finding extends the validity of the shell model to neutron-rich nuclei, and provides a benchmark for predicting the properties of nuclei even farther from stability, including those involved in neutron-capture reactions in supernovae.
Atomic nuclei have a shell structure that allows for 'magic numbers' of neutrons and protons, analogous to the noble gases in atomic physics. Knowledge of the properties of single-particle states outside nuclear shell closures in exotic nuclei is important for the fundamental understanding of nuclear structure and nucleosynthesis. Here, a nucleon-transfer technique has been used to measure the single-particle states of
133
Sn, revealing the highly magic nature of
132
Sn.
Atomic nuclei have a shell structure
1
in which nuclei with ‘magic numbers’ of neutrons and protons are analogous to the noble gases in atomic physics. Only ten nuclei with the standard magic numbers of both neutrons and protons have so far been observed. The nuclear shell model is founded on the precept that neutrons and protons can move as independent particles in orbitals with discrete quantum numbers, subject to a mean field generated by all the other nucleons. Knowledge of the properties of single-particle states outside nuclear shell closures in exotic nuclei is important
2
,
3
,
4
,
5
for a fundamental understanding of nuclear structure and nucleosynthesis (for example the r-process, which is responsible for the production of about half of the heavy elements). However, as a result of their short lifetimes, there is a paucity of knowledge about the nature of single-particle states outside exotic doubly magic nuclei. Here we measure the single-particle character of the levels in
133
Sn that lie outside the double shell closure present at the short-lived nucleus
132
Sn. We use an inverse kinematics technique that involves the transfer of a single nucleon to the nucleus. The purity of the measured single-particle states clearly illustrates the magic nature of
132
Sn. Atomic nuclei have a shell structure1 in which nuclei with magic numbers of neutrons and protons are analogous to the noble gases in atomic physics. Only ten nuclei with the standard magic numbers of both neutrons and protons have so far been observed. The nuclear shell model is founded on the precept that neutrons and protons can move as independent particles in orbitals with discrete quantum numbers, subject to a mean field generated by all the other nucleons. Knowledge of the properties of single-particle states outside nuclear shell closures in exotic nuclei is important2 5 for a fundamental understanding of nuclear structure and nucleosynthesis (for example the r-process, which is responsible for the production of about half of the heavy elements). However, as a result of their short lifetimes, there is a paucity of knowledge about the nature of single-particle states outside exotic doubly magic nuclei. Here we measure the single-particle character of the levels in 133Sn that lies outside the double shell closure present at the short-lived nucleus 132Sn. We use an inverse kinematics technique that involves the transfer of a single nucleon to the nucleus. The purity of the measured single-particle states clearly illustrates the magic nature of 132Sn. |
Author | Swan, T. P. Liang, J. F. Nesaraja, C. D. Cizewski, J. A. Shriner, J. F. Smith, M. S. Chipps, K. A. Erikson, L. Shapira, D. Thomas, J. S. Kapler, R. Bardayan, D. W. Jones, K. L. Nunes, F. M. Patterson, N. P. Chae, K. Y. Ma, Z. Adekola, A. S. Pain, S. D. Hatarik, R. Livesay, R. Harlin, C. Kozub, R. L. Blackmon, J. C. Moazen, B. H. |
Author_xml | – sequence: 1 givenname: K. L. surname: Jones fullname: Jones, K. L. email: kgrzywac@utk.edu organization: Department of Physics and Astronomy, University of Tennessee, Knoxville, Tennessee 37996, USA, Department of Physics and Astronomy, Rutgers University, New Brunswick, New Jersey 08903, USA – sequence: 2 givenname: A. S. surname: Adekola fullname: Adekola, A. S. organization: Department of Physics and Astronomy, Ohio University, Athens, Ohio 45701, USA – sequence: 3 givenname: D. W. surname: Bardayan fullname: Bardayan, D. W. organization: Physics Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA – sequence: 4 givenname: J. C. surname: Blackmon fullname: Blackmon, J. C. organization: Physics Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA – sequence: 5 givenname: K. Y. surname: Chae fullname: Chae, K. Y. organization: Department of Physics and Astronomy, University of Tennessee, Knoxville, Tennessee 37996, USA – sequence: 6 givenname: K. A. surname: Chipps fullname: Chipps, K. A. organization: Physics Department, Colorado School of Mines, Golden, Colorado 80401, USA – sequence: 7 givenname: J. A. surname: Cizewski fullname: Cizewski, J. A. organization: Department of Physics and Astronomy, Rutgers University, New Brunswick, New Jersey 08903, USA – sequence: 8 givenname: L. surname: Erikson fullname: Erikson, L. organization: Physics Department, Colorado School of Mines, Golden, Colorado 80401, USA – sequence: 9 givenname: C. surname: Harlin fullname: Harlin, C. organization: Department of Physics, University of Surrey, Guildford, Surrey GU2 7XH, UK – sequence: 10 givenname: R. surname: Hatarik fullname: Hatarik, R. organization: Department of Physics and Astronomy, Rutgers University, New Brunswick, New Jersey 08903, USA – sequence: 11 givenname: R. surname: Kapler fullname: Kapler, R. organization: Department of Physics and Astronomy, University of Tennessee, Knoxville, Tennessee 37996, USA – sequence: 12 givenname: R. L. surname: Kozub fullname: Kozub, R. L. organization: Department of Physics, Tennessee Technological University, Cookeville, Tennessee 38505, USA – sequence: 13 givenname: J. F. surname: Liang fullname: Liang, J. F. organization: Physics Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA – sequence: 14 givenname: R. surname: Livesay fullname: Livesay, R. organization: Physics Department, Colorado School of Mines, Golden, Colorado 80401, USA – sequence: 15 givenname: Z. surname: Ma fullname: Ma, Z. organization: Department of Physics and Astronomy, University of Tennessee, Knoxville, Tennessee 37996, USA – sequence: 16 givenname: B. H. surname: Moazen fullname: Moazen, B. H. organization: Department of Physics and Astronomy, University of Tennessee, Knoxville, Tennessee 37996, USA – sequence: 17 givenname: C. D. surname: Nesaraja fullname: Nesaraja, C. D. organization: Physics Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA – sequence: 18 givenname: F. M. surname: Nunes fullname: Nunes, F. M. organization: National Superconducting Cyclotron Laboratory and Department of Physics and Astronomy, Michigan State University, East Lansing, Michigan 48824, USA – sequence: 19 givenname: S. D. surname: Pain fullname: Pain, S. D. organization: Department of Physics and Astronomy, Rutgers University, New Brunswick, New Jersey 08903, USA – sequence: 20 givenname: N. P. surname: Patterson fullname: Patterson, N. P. organization: Department of Physics, University of Surrey, Guildford, Surrey GU2 7XH, UK – sequence: 21 givenname: D. surname: Shapira fullname: Shapira, D. organization: Physics Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA – sequence: 22 givenname: J. F. surname: Shriner fullname: Shriner, J. F. organization: Department of Physics, Tennessee Technological University, Cookeville, Tennessee 38505, USA – sequence: 23 givenname: M. S. surname: Smith fullname: Smith, M. S. organization: Physics Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA – sequence: 24 givenname: T. P. surname: Swan fullname: Swan, T. P. organization: Department of Physics and Astronomy, Rutgers University, New Brunswick, New Jersey 08903, USA, Department of Physics, University of Surrey, Guildford, Surrey GU2 7XH, UK – sequence: 25 givenname: J. S. surname: Thomas fullname: Thomas, J. S. organization: Department of Physics, University of Surrey, Guildford, Surrey GU2 7XH, UK |
BackLink | http://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=22796934$$DView record in Pascal Francis https://www.osti.gov/biblio/985782$$D View this record in Osti.gov |
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ContentType | Journal Article |
Copyright | Macmillan Publishers Limited. All rights reserved 2010 2015 INIST-CNRS |
Copyright_xml | – notice: Macmillan Publishers Limited. All rights reserved 2010 – notice: 2015 INIST-CNRS |
CorporateAuthor | Oak Ridge National Lab. (ORNL), Oak Ridge, TN (United States) Holifield Radioactive Ion Beam Facility |
CorporateAuthor_xml | – name: Oak Ridge National Lab. (ORNL), Oak Ridge, TN (United States) – name: Holifield Radioactive Ion Beam Facility |
DBID | AAYXX CITATION IQODW OTOTI |
DOI | 10.1038/nature09048 |
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Discipline | Sciences (General) Physics |
EISSN | 1476-4687 |
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Keywords | Protons Nuclear structure Magic nuclei Quantum numbers Nuclear shell model Nucleosynthesis Neutrons r process Heavy element Lifetime Atomic nucleus Magic number Kinematics Tin Nucleons |
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References_xml | – reference: GraweHLangankeKMartínez-PinedoGNuclear structure and astrophysicsRep. Prog. Phys.200770152515822007RPPh...70.1525G1:CAS:528:DC%2BD2sXhtF2hsrbN10.1088/0034-4885/70/9/R02 – reference: HoffPSingle-neutron states in 133SnPhys. Rev. Lett.199677102010231996PhRvL..77.1020H1:CAS:528:DyaK28XltFWlsLg%3D10.1103/PhysRevLett.77.1020 – reference: BarbieriCHjorth-JensenMQuasiparticle and quasihole states of nuclei around 56NiPhys. Rev. C2009790643132009PhRvC..79f4313B10.1103/PhysRevC.79.064313 – reference: KozubRLNeutron single particle strengths from the (d,p) reaction on 18FPhys. Rev. C2006730443072006PhRvC..73d4307K10.1103/PhysRevC.73.044307 – reference: CoraggioLCovelloAGarganoAItacoNSimilarity of nuclear structure in the 132Sn and 208Pb regions: proton–neutron multipletsPhys. Rev. C200980021305(R)2009PhRvC..80b1305C10.1103/PhysRevC.80.021305 – reference: EllegaardCKanteleJVedelsbyPParticle–vibration coupling in 209PbNucl. Phys. A19691291131281969NuPhA.129..113E1:CAS:528:DyaF1MXktVyltbY%3D10.1016/0375-9474(69)90912-9 – reference: CowanJJThielemannF-KTruranJWThe r-process and nucleochronologyPhys. Rep.19912082673941991PhR...208..267C1:CAS:528:DyaK38XivV2mtQ%3D%3D10.1016/0370-1573(91)90070-3 – reference: RehmKEStudy of the 56Ni(d,p)57Ni reaction and the astrophysical 56Ni(p,γ)57Cu reaction ratePhys. Rev. Lett.1998806766791998PhRvL..80..676R1:CAS:528:DyaK1cXlsVOqtg%3D%3D10.1103/PhysRevLett.80.676 – reference: MayerMGJensenJHDTheory of Nuclear Shell Structure19550065.23203 – reference: StracenerDWStatus of radioactive ion beams at the HRIBFNucl. Instrum. Methods A20045211261352004NIMPA.521..126S1:CAS:528:DC%2BD2cXitlyjsr0%3D10.1016/j.nima.2003.11.142 – reference: WizaJLMicrochannel plate detectorsNucl. Instrum. Methods19791625876011979NucIM.162..587L1:CAS:528:DyaE1MXkvFyisb4%3D10.1016/0029-554X(79)90734-1 – reference: ReidRVLocal phenomenological nucleon–nucleon potentialsAnn. Phys.1968504114481968AnPhy..50..411R10.1016/0003-4916(68)90126-7 – reference: ThompsonIJCoupled reaction channels calculations in nuclear physicsComput. Phys. Rep.198871672111988CoPhR...7..167T1:CAS:528:DyaL1cXit1OktbY%3D10.1016/0167-7977(88)90005-6 – reference: UrbanWNeutron single-particle energies in the 132Sn regionEur. Phys. J. A199952392411999EPJA....5..239U1:CAS:528:DyaK1MXkslSjurc%3D10.1007/s100500050280 – reference: KartamyshevMPEngelandTHjorth-JensenMOsnesEEffective Interactions and shell model studies of heavy tin isotopesPhys. Rev. C2007760243132007PhRvC..76b4313K10.1103/PhysRevC.76.024313 – reference: TerasakiJEngelJNazarewiczWStoitsovMAnomalous behavior of 2+ excitations around 132SnPhys. Rev. C2002660543132002PhRvC..66e4313T10.1103/PhysRevC.66.054313 – reference: HirotaKAokiYOkumuraNTagishiYDeuteron elastic scattering and (d,p) reactions on 208Pb at Ed = 22 MeV and j-dependence of T20 in (d,p) reactionNucl. Phys. A19986285475791998NuPhA.628..547H10.1016/S0375-9474(97)00641-6 – reference: SarkarSSarkarMSShell model study of neutron-rich nuclei near 132SnPhys. Rev. C2001640143122001PhRvC..64a4312S10.1103/PhysRevC.64.014312 – reference: PainSDDevelopment of a high solid-angle silicon detector array for measurement of transfer reactions in inverse kinematicsNucl. Instrum. Methods B2007261112211252007NIMPB.261.1122P1:CAS:528:DC%2BD2sXnslSmt74%3D10.1016/j.nimb.2007.04.289 – reference: ThomasJSSingle-neutron excitations in neutron-rich 83Ge and 85SePhys. Rev. C2007760443022007PhRvC..76d4302T10.1103/PhysRevC.76.044302 – reference: PangDYNunesFMMukhamedzhanovAMAre spectroscopic factors from transfer reactions consistent with asymptotic normalization coefficients?Phys. Rev. C2007750246012007PhRvC..75b4601P10.1103/PhysRevC.75.024601 – reference: StrömichA(d,p) reactions on 124Sn, 130Te, 138Ba, 140Ce, 142Nd, and 208Pb below and near the Coulomb barrierPhys. Rev. C197716219322071977PhRvC..16.2193S10.1103/PhysRevC.16.2193 – reference: KramerGJBlokHPLapikásLA consistent analysis of (e,e′p) and (d,3He) experimentsNucl. Phys. A20016792672862001NuPhA.679..267K10.1016/S0375-9474(00)00379-1 – volume: 70 start-page: 1525 year: 2007 ident: BFnature09048_CR5 publication-title: Rep. Prog. Phys. doi: 10.1088/0034-4885/70/9/R02 – volume: 521 start-page: 126 year: 2004 ident: BFnature09048_CR14 publication-title: Nucl. Instrum. Methods A doi: 10.1016/j.nima.2003.11.142 – volume: 5 start-page: 239 year: 1999 ident: BFnature09048_CR10 publication-title: Eur. Phys. J. A doi: 10.1007/s100500050280 – volume: 79 start-page: 064313 year: 2009 ident: BFnature09048_CR2 publication-title: Phys. Rev. C doi: 10.1103/PhysRevC.79.064313 – volume: 76 start-page: 024313 year: 2007 ident: BFnature09048_CR3 publication-title: Phys. Rev. C doi: 10.1103/PhysRevC.76.024313 – volume: 162 start-page: 587 year: 1979 ident: BFnature09048_CR16 publication-title: Nucl. Instrum. 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Snippet | Nuclear magic
Atomic nuclei have a shell structure that allows for 'magic' numbers of neutrons and protons, analogous to the noble gases in atomic physics.... Atomic nuclei have a shell structure1 in which nuclei with magic numbers of neutrons and protons are analogous to the noble gases in atomic physics. Only ten... |
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SubjectTerms | 639/638/263 639/766/387 ATOMIC AND MOLECULAR PHYSICS ATOMIC PHYSICS CLASSICAL AND QUANTUM MECHANICS, GENERAL PHYSICS CLOSURES Exact sciences and technology Humanities and Social Sciences letter MAGIC NUCLEI multidisciplinary NEUTRONS Nuclear physics NUCLEAR PHYSICS AND RADIATION PHYSICS NUCLEAR STRUCTURE NUCLEI NUCLEONS NUCLEOSYNTHESIS Physics PHYSICS OF ELEMENTARY PARTICLES AND FIELDS PRODUCTION PROTONS QUANTUM NUMBERS R PROCESS RARE GASES Science SHELL MODELS |
Title | The magic nature of 132Sn explored through the single-particle states of 133Sn |
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