减少富中子核中 Z=8 外壳上的光谱重叠

IF 3.2 2区 物理与天体物理 Q2 PHYSICS, NUCLEAR
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. 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引用次数: 0

摘要

最近对 O27 和 O28 的发现和光谱测量表明,这些富中子氧同位素的 N=20 壳结构已经消失。我们分别测量了 F27 和 Ne29 的一质子和二质子去除截面,提取了光谱因子,并将其与壳模型重叠函数和 eikonal 反应模型计算结果进行了比较。利用不变质量技术重建了撞击 Be9 靶的 F27(106.2 MeV/u)和 Ne29(112.8 MeV/u)光束的敲除反应的二体(O24+n)和三体(O24+2n)衰变能量。来自 F27 的单质子去除强烈填充了 O26 的基态,提取的横截面为 3.4-1.5+0.3 mb,与 eikonal 模型的计算结果一致,这些计算结果通过壳模型光谱因子归一化,并考虑了在所用模型中观察到的单核子去除反应的系统性降低因子。在 Ne29 的双质子去除反应中,通过 O26 的基态衰变的 O27 中的填充态提取的上限为 0.08 mb。从 Ne29 的双质子去除反应中测得的 O26 基态群上限表明 F27 和 Ne29 的基本核结构存在显著差异。
本文章由计算机程序翻译,如有差异,请以英文原文为准。

Reduction of spectroscopic overlap across the 
<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>
 shell in neutron-rich nuclei

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 3.41.5+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
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来源期刊
Physical Review C
Physical Review C PHYSICS, NUCLEAR-
CiteScore
5.80
自引率
35.50%
发文量
863
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
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