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":3,"journal":{"name":"ACS Applied Electronic Materials","volume":"11 47","pages":""},"PeriodicalIF":4.7000,"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\":3,\"journal\":{\"name\":\"ACS Applied Electronic Materials\",\"volume\":\"11 47\",\"pages\":\"\"},\"PeriodicalIF\":4.7000,\"publicationDate\":\"2024-05-24\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"ACS Applied Electronic Materials\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://doi.org/10.1103/physrevc.109.054325\",\"RegionNum\":3,\"RegionCategory\":\"材料科学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q1\",\"JCRName\":\"ENGINEERING, ELECTRICAL & ELECTRONIC\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"ACS Applied Electronic Materials","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1103/physrevc.109.054325","RegionNum":3,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"ENGINEERING, ELECTRICAL & ELECTRONIC","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:
ACS Applied Electronic Materials is an interdisciplinary journal publishing original research covering all aspects of electronic materials. The journal is devoted to reports of new and original experimental and theoretical research of an applied nature that integrate knowledge in the areas of materials science, engineering, optics, physics, and chemistry into important applications of electronic materials. Sample research topics that span the journal's scope are inorganic, organic, ionic and polymeric materials with properties that include conducting, semiconducting, superconducting, insulating, dielectric, magnetic, optoelectronic, piezoelectric, ferroelectric and thermoelectric.
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