T. Redpath, P. Guèye, T. Baumann, B. A. Brown, A. Cunningham, P. A. DeYoung, N. Frank, C. R. Hoffman, A. N. Kuchera, B. Monteagudo Godoy, C. Persch, A. Revel, W. F. Rogers, M. Thoennessen, J. A. Tostevin, D. Votaw
{"title":"减少富中子核中 Z=8 外壳上的光谱重叠","authors":"T. Redpath, P. Guèye, T. Baumann, B. A. Brown, A. Cunningham, P. A. DeYoung, N. Frank, C. R. Hoffman, A. N. Kuchera, B. Monteagudo Godoy, C. Persch, A. Revel, W. F. Rogers, M. Thoennessen, J. A. Tostevin, D. Votaw","doi":"10.1103/physrevc.109.054325","DOIUrl":null,"url":null,"abstract":"<jats:p> The recent discovery and spectroscopic measurements of <a:math xmlns:a=\"http://www.w3.org/1998/Math/MathML\"><a:mmultiscripts><a:mi mathvariant=\"normal\">O</a:mi><a:mprescripts/><a:none/><a:mn>27</a:mn></a:mmultiscripts></a:math> and <c:math xmlns:c=\"http://www.w3.org/1998/Math/MathML\"><c:mmultiscripts><c:mi mathvariant=\"normal\">O</c:mi><c:mprescripts/><c:none/><c:mn>28</c:mn></c:mmultiscripts></c:math> suggests the disappearance of the <e:math xmlns:e=\"http://www.w3.org/1998/Math/MathML\"><e:mrow><e:mi>N</e:mi><e:mo>=</e:mo><e:mn>20</e:mn></e:mrow></e:math> shell structure in these neutron-rich oxygen isotopes.</jats:p>\n<jats:p> We measured one- and two-proton removal cross sections from <f:math xmlns:f=\"http://www.w3.org/1998/Math/MathML\"><f:mmultiscripts><f:mi mathvariant=\"normal\">F</f:mi><f:mprescripts/><f:none/><f:mn>27</f:mn></f:mmultiscripts></f:math> and <h:math xmlns:h=\"http://www.w3.org/1998/Math/MathML\"><h:mmultiscripts><h:mi>Ne</h:mi><h:mprescripts/><h:none/><h:mn>29</h:mn></h:mmultiscripts></h:math>, respectively, extracting spectroscopic factors and comparing them to shell model overlap functions coupled with eikonal reaction model calculations.</jats:p>\n<jats:p> The invariant mass technique was used to reconstruct the two-body (<i:math xmlns:i=\"http://www.w3.org/1998/Math/MathML\"><i:mrow><i:mmultiscripts><i:mi mathvariant=\"normal\">O</i:mi><i:mprescripts/><i:none/><i:mn>24</i:mn></i:mmultiscripts><i:mo>+</i:mo><i:mi>n</i:mi></i:mrow></i:math>) and three-body (<k:math xmlns:k=\"http://www.w3.org/1998/Math/MathML\"><k:mrow><k:mmultiscripts><k:mi mathvariant=\"normal\">O</k:mi><k:mprescripts/><k:none/><k:mn>24</k:mn></k:mmultiscripts><k:mo>+</k:mo><k:mn>2</k:mn><k:mi>n</k:mi></k:mrow></k:math>) decay energies from knockout reactions of <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"><m:mmultiscripts><m:mi mathvariant=\"normal\">F</m:mi><m:mprescripts/><m:none/><m:mn>27</m:mn></m:mmultiscripts></m:math> (106.2 MeV/u) and <o:math xmlns:o=\"http://www.w3.org/1998/Math/MathML\"><o:mmultiscripts><o:mi>Ne</o:mi><o:mprescripts/><o:none/><o:mn>29</o:mn></o:mmultiscripts></o:math> (112.8 MeV/u) beams impinging on a <p:math xmlns:p=\"http://www.w3.org/1998/Math/MathML\"><p:mmultiscripts><p:mi>Be</p:mi><p:mprescripts/><p:none/><p:mn>9</p:mn></p:mmultiscripts></p:math> target.</jats:p>\n<jats:p> The one-proton removal from <q:math xmlns:q=\"http://www.w3.org/1998/Math/MathML\"><q:mmultiscripts><q:mi mathvariant=\"normal\">F</q:mi><q:mprescripts/><q:none/><q:mn>27</q:mn></q:mmultiscripts></q:math> strongly populated the ground state of <s:math xmlns:s=\"http://www.w3.org/1998/Math/MathML\"><s:mmultiscripts><s:mi mathvariant=\"normal\">O</s:mi><s:mprescripts/><s:none/><s:mn>26</s:mn></s:mmultiscripts></s:math> and the extracted cross section of <u:math xmlns:u=\"http://www.w3.org/1998/Math/MathML\"><u:mrow><u:mn>3</u:mn><u:mo>.</u:mo><u:msubsup><u:mn>4</u:mn><u:mrow><u:mo>−</u:mo><u:mn>1.5</u:mn></u:mrow><u:mrow><u:mo>+</u:mo><u:mn>0.3</u:mn></u:mrow></u:msubsup></u:mrow></u:math> mb agrees with eikonal model calculations that are normalized by the shell model spectroscopic factors and account for the systematic reduction factor observed for single nucleon removal reactions within the models used. For the two-proton removal reaction from <v:math xmlns:v=\"http://www.w3.org/1998/Math/MathML\"><v:mmultiscripts><v:mi>Ne</v:mi><v:mprescripts/><v:none/><v:mn>29</v:mn></v:mmultiscripts></v:math> an upper limit of 0.08 mb was extracted for populating states in <w:math xmlns:w=\"http://www.w3.org/1998/Math/MathML\"><w:mmultiscripts><w:mi mathvariant=\"normal\">O</w:mi><w:mprescripts/><w:none/><w:mn>27</w:mn></w:mmultiscripts></w:math> decaying though the ground state of <y:math xmlns:y=\"http://www.w3.org/1998/Math/MathML\"><y:mmultiscripts><y:mi mathvariant=\"normal\">O</y:mi><y:mprescripts/><y:none/><y:mn>26</y:mn></y:mmultiscripts></y:math>.</jats:p>\n<jats:p> The measured upper limit for the population of the ground state of <ab:math xmlns:ab=\"http://www.w3.org/1998/Math/MathML\"><ab:mmultiscripts><ab:mi mathvariant=\"normal\">O</ab:mi><ab:mprescripts/><ab:none/><ab:mn>26</ab:mn></ab:mmultiscripts></ab:math> in the two-proton removal reaction from <cb:math xmlns:cb=\"http://www.w3.org/1998/Math/MathML\"><cb:mmultiscripts><cb:mi>Ne</cb:mi><cb:mprescripts/><cb:none/><cb:mn>29</cb:mn></cb:mmultiscripts></cb:math> indicates a significant difference in the underlying nuclear structure of <db:math xmlns:db=\"http://www.w3.org/1998/Math/MathML\"><db:mmultiscripts><db:mi mathvariant=\"normal\">F</db:mi><db:mprescripts/><db:none/><db:mn>27</db:mn></db:mmultiscripts></db:math> and <fb:math xmlns:fb=\"http://www.w3.org/1998/Math/MathML\"><fb:mmultiscripts><fb:mi>Ne</fb:mi><fb:mprescripts/><fb:none/><fb:mn>29</fb:mn></fb:mmultiscripts></fb:math>.</jats:p><jats:sec><jats:title/><jats:supplementary-material><jats:permissions><jats:copyright-statement>Published by the American Physical Society</jats:copyright-statement><jats:copyright-year>2024</jats:copyright-year></jats:permissions></jats:supplementary-material></jats:sec>","PeriodicalId":48700,"journal":{"name":"Physical Review C","volume":null,"pages":null},"PeriodicalIF":3.2000,"publicationDate":"2024-05-24","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Reduction of spectroscopic overlap across the \\n<mml:math xmlns:mml=\\\"http://www.w3.org/1998/Math/MathML\\\"><mml:mrow><mml:mi>Z</mml:mi><mml:mo>=</mml:mo><mml:mn>8</mml:mn></mml:mrow></mml:math>\\n shell in neutron-rich nuclei\",\"authors\":\"T. Redpath, P. Guèye, T. Baumann, B. A. Brown, A. Cunningham, P. A. DeYoung, N. Frank, C. R. Hoffman, A. N. Kuchera, B. Monteagudo Godoy, C. Persch, A. Revel, W. F. Rogers, M. Thoennessen, J. A. Tostevin, D. Votaw\",\"doi\":\"10.1103/physrevc.109.054325\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<jats:p> The recent discovery and spectroscopic measurements of <a:math xmlns:a=\\\"http://www.w3.org/1998/Math/MathML\\\"><a:mmultiscripts><a:mi mathvariant=\\\"normal\\\">O</a:mi><a:mprescripts/><a:none/><a:mn>27</a:mn></a:mmultiscripts></a:math> and <c:math xmlns:c=\\\"http://www.w3.org/1998/Math/MathML\\\"><c:mmultiscripts><c:mi mathvariant=\\\"normal\\\">O</c:mi><c:mprescripts/><c:none/><c:mn>28</c:mn></c:mmultiscripts></c:math> suggests the disappearance of the <e:math xmlns:e=\\\"http://www.w3.org/1998/Math/MathML\\\"><e:mrow><e:mi>N</e:mi><e:mo>=</e:mo><e:mn>20</e:mn></e:mrow></e:math> shell structure in these neutron-rich oxygen isotopes.</jats:p>\\n<jats:p> We measured one- and two-proton removal cross sections from <f:math xmlns:f=\\\"http://www.w3.org/1998/Math/MathML\\\"><f:mmultiscripts><f:mi mathvariant=\\\"normal\\\">F</f:mi><f:mprescripts/><f:none/><f:mn>27</f:mn></f:mmultiscripts></f:math> and <h:math xmlns:h=\\\"http://www.w3.org/1998/Math/MathML\\\"><h:mmultiscripts><h:mi>Ne</h:mi><h:mprescripts/><h:none/><h:mn>29</h:mn></h:mmultiscripts></h:math>, respectively, extracting spectroscopic factors and comparing them to shell model overlap functions coupled with eikonal reaction model calculations.</jats:p>\\n<jats:p> The invariant mass technique was used to reconstruct the two-body (<i:math xmlns:i=\\\"http://www.w3.org/1998/Math/MathML\\\"><i:mrow><i:mmultiscripts><i:mi mathvariant=\\\"normal\\\">O</i:mi><i:mprescripts/><i:none/><i:mn>24</i:mn></i:mmultiscripts><i:mo>+</i:mo><i:mi>n</i:mi></i:mrow></i:math>) and three-body (<k:math xmlns:k=\\\"http://www.w3.org/1998/Math/MathML\\\"><k:mrow><k:mmultiscripts><k:mi mathvariant=\\\"normal\\\">O</k:mi><k:mprescripts/><k:none/><k:mn>24</k:mn></k:mmultiscripts><k:mo>+</k:mo><k:mn>2</k:mn><k:mi>n</k:mi></k:mrow></k:math>) decay energies from knockout reactions of <m:math xmlns:m=\\\"http://www.w3.org/1998/Math/MathML\\\"><m:mmultiscripts><m:mi mathvariant=\\\"normal\\\">F</m:mi><m:mprescripts/><m:none/><m:mn>27</m:mn></m:mmultiscripts></m:math> (106.2 MeV/u) and <o:math xmlns:o=\\\"http://www.w3.org/1998/Math/MathML\\\"><o:mmultiscripts><o:mi>Ne</o:mi><o:mprescripts/><o:none/><o:mn>29</o:mn></o:mmultiscripts></o:math> (112.8 MeV/u) beams impinging on a <p:math xmlns:p=\\\"http://www.w3.org/1998/Math/MathML\\\"><p:mmultiscripts><p:mi>Be</p:mi><p:mprescripts/><p:none/><p:mn>9</p:mn></p:mmultiscripts></p:math> target.</jats:p>\\n<jats:p> The one-proton removal from <q:math xmlns:q=\\\"http://www.w3.org/1998/Math/MathML\\\"><q:mmultiscripts><q:mi mathvariant=\\\"normal\\\">F</q:mi><q:mprescripts/><q:none/><q:mn>27</q:mn></q:mmultiscripts></q:math> strongly populated the ground state of <s:math xmlns:s=\\\"http://www.w3.org/1998/Math/MathML\\\"><s:mmultiscripts><s:mi mathvariant=\\\"normal\\\">O</s:mi><s:mprescripts/><s:none/><s:mn>26</s:mn></s:mmultiscripts></s:math> and the extracted cross section of <u:math xmlns:u=\\\"http://www.w3.org/1998/Math/MathML\\\"><u:mrow><u:mn>3</u:mn><u:mo>.</u:mo><u:msubsup><u:mn>4</u:mn><u:mrow><u:mo>−</u:mo><u:mn>1.5</u:mn></u:mrow><u:mrow><u:mo>+</u:mo><u:mn>0.3</u:mn></u:mrow></u:msubsup></u:mrow></u:math> mb agrees with eikonal model calculations that are normalized by the shell model spectroscopic factors and account for the systematic reduction factor observed for single nucleon removal reactions within the models used. For the two-proton removal reaction from <v:math xmlns:v=\\\"http://www.w3.org/1998/Math/MathML\\\"><v:mmultiscripts><v:mi>Ne</v:mi><v:mprescripts/><v:none/><v:mn>29</v:mn></v:mmultiscripts></v:math> an upper limit of 0.08 mb was extracted for populating states in <w:math xmlns:w=\\\"http://www.w3.org/1998/Math/MathML\\\"><w:mmultiscripts><w:mi mathvariant=\\\"normal\\\">O</w:mi><w:mprescripts/><w:none/><w:mn>27</w:mn></w:mmultiscripts></w:math> decaying though the ground state of <y:math xmlns:y=\\\"http://www.w3.org/1998/Math/MathML\\\"><y:mmultiscripts><y:mi mathvariant=\\\"normal\\\">O</y:mi><y:mprescripts/><y:none/><y:mn>26</y:mn></y:mmultiscripts></y:math>.</jats:p>\\n<jats:p> The measured upper limit for the population of the ground state of <ab:math xmlns:ab=\\\"http://www.w3.org/1998/Math/MathML\\\"><ab:mmultiscripts><ab:mi mathvariant=\\\"normal\\\">O</ab:mi><ab:mprescripts/><ab:none/><ab:mn>26</ab:mn></ab:mmultiscripts></ab:math> in the two-proton removal reaction from <cb:math xmlns:cb=\\\"http://www.w3.org/1998/Math/MathML\\\"><cb:mmultiscripts><cb:mi>Ne</cb:mi><cb:mprescripts/><cb:none/><cb:mn>29</cb:mn></cb:mmultiscripts></cb:math> indicates a significant difference in the underlying nuclear structure of <db:math xmlns:db=\\\"http://www.w3.org/1998/Math/MathML\\\"><db:mmultiscripts><db:mi mathvariant=\\\"normal\\\">F</db:mi><db:mprescripts/><db:none/><db:mn>27</db:mn></db:mmultiscripts></db:math> and <fb:math xmlns:fb=\\\"http://www.w3.org/1998/Math/MathML\\\"><fb:mmultiscripts><fb:mi>Ne</fb:mi><fb:mprescripts/><fb:none/><fb:mn>29</fb:mn></fb:mmultiscripts></fb:math>.</jats:p><jats:sec><jats:title/><jats:supplementary-material><jats:permissions><jats:copyright-statement>Published by the American Physical Society</jats:copyright-statement><jats:copyright-year>2024</jats:copyright-year></jats:permissions></jats:supplementary-material></jats:sec>\",\"PeriodicalId\":48700,\"journal\":{\"name\":\"Physical Review C\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":3.2000,\"publicationDate\":\"2024-05-24\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Physical Review C\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://doi.org/10.1103/physrevc.109.054325\",\"RegionNum\":2,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"PHYSICS, NUCLEAR\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Physical Review C","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1103/physrevc.109.054325","RegionNum":2,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"PHYSICS, NUCLEAR","Score":null,"Total":0}
Reduction of spectroscopic overlap across the
Z=8
shell in neutron-rich nuclei
The recent discovery and spectroscopic measurements of O27 and O28 suggests the disappearance of the N=20 shell structure in these neutron-rich oxygen isotopes. We measured one- and two-proton removal cross sections from F27 and Ne29, respectively, extracting spectroscopic factors and comparing them to shell model overlap functions coupled with eikonal reaction model calculations. The invariant mass technique was used to reconstruct the two-body (O24+n) and three-body (O24+2n) decay energies from knockout reactions of F27 (106.2 MeV/u) and Ne29 (112.8 MeV/u) beams impinging on a Be9 target. The one-proton removal from F27 strongly populated the ground state of O26 and the extracted cross section of 3.4−1.5+0.3 mb agrees with eikonal model calculations that are normalized by the shell model spectroscopic factors and account for the systematic reduction factor observed for single nucleon removal reactions within the models used. For the two-proton removal reaction from Ne29 an upper limit of 0.08 mb was extracted for populating states in O27 decaying though the ground state of O26. The measured upper limit for the population of the ground state of O26 in the two-proton removal reaction from Ne29 indicates a significant difference in the underlying nuclear structure of F27 and Ne29.Published by the American Physical Society2024
期刊介绍:
Physical Review C (PRC) is a leading journal in theoretical and experimental nuclear physics, publishing more than two-thirds of the research literature in the field.
PRC covers experimental and theoretical results in all aspects of nuclear physics, including:
Nucleon-nucleon interaction, few-body systems
Nuclear structure
Nuclear reactions
Relativistic nuclear collisions
Hadronic physics and QCD
Electroweak interaction, symmetries
Nuclear astrophysics