违反同位旋衰变Ds*→Dsπ0和中间介子环辐射衰变Ds*→Dsγ的联合研究

IF 5.3 2区 物理与天体物理 Q1 Physics and Astronomy
Jun Wang, Qiang Zhao
{"title":"违反同位旋衰变Ds*→Dsπ0和中间介子环辐射衰变Ds*→Dsγ的联合研究","authors":"Jun Wang, Qiang Zhao","doi":"10.1103/physrevd.111.096007","DOIUrl":null,"url":null,"abstract":"We carry out a combined study of the isospin-violating decay D</a:mi></a:mrow>s</a:mi></a:mrow>*</a:mo></a:mrow></a:msubsup>→</a:mo>D</a:mi></a:mrow>s</a:mi></a:mrow></a:msub>π</a:mi></a:mrow>0</a:mn></a:mrow></a:msup></a:mrow></a:math> and radiative decay <d:math xmlns:d=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><d:msubsup><d:mi>D</d:mi><d:mi>s</d:mi><d:mo>*</d:mo></d:msubsup><d:mo stretchy=\"false\">→</d:mo><d:msub><d:mi>D</d:mi><d:mi>s</d:mi></d:msub><d:mi>γ</d:mi></d:math> in an effective Lagrangian approach by taking into account the corrections from the one-loop transitions. By distinguishing the transition mechanisms of the long-distance interactions through the intermediate meson loops from the short-distance interactions through the <g:math xmlns:g=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><g:mi>η</g:mi><g:mo>−</g:mo><g:msup><g:mi>π</g:mi><g:mn>0</g:mn></g:msup></g:math> mixing at the tree level, the isospin-violating decay <i:math xmlns:i=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><i:msubsup><i:mi>D</i:mi><i:mi>s</i:mi><i:mo>*</i:mo></i:msubsup><i:mo stretchy=\"false\">→</i:mo><i:msub><i:mi>D</i:mi><i:mi>s</i:mi></i:msub><i:msup><i:mi>π</i:mi><i:mn>0</i:mn></i:msup></i:math> can be well constrained. In our approach, the higher-order corrections to the isospin-violating effects can involve the intermediate <l:math xmlns:l=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><l:msup><l:mi>D</l:mi><l:mrow><l:mo stretchy=\"false\">(</l:mo><l:mo>*</l:mo><l:mo stretchy=\"false\">)</l:mo></l:mrow></l:msup></l:math> and <p:math xmlns:p=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><p:msup><p:mi>K</p:mi><p:mrow><p:mo stretchy=\"false\">(</p:mo><p:mo>*</p:mo><p:mo stretchy=\"false\">)</p:mo></p:mrow></p:msup></p:math> scatterings. We find that the contributions from the destructive interference of intermediate meson loops via <t:math xmlns:t=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><t:mrow><t:msup><t:mrow><t:mi>D</t:mi></t:mrow><t:mrow><t:mo stretchy=\"false\">(</t:mo><t:mo>*</t:mo><t:mo stretchy=\"false\">)</t:mo><t:mn>0</t:mn></t:mrow></t:msup><t:mo stretchy=\"false\">(</t:mo><t:mi>c</t:mi><t:mover accent=\"true\"><t:mrow><t:mi>u</t:mi></t:mrow><t:mrow><t:mo stretchy=\"false\">¯</t:mo></t:mrow></t:mover><t:mo stretchy=\"false\">)</t:mo><t:msup><t:mrow><t:mi>K</t:mi></t:mrow><t:mrow><t:mo stretchy=\"false\">(</t:mo><t:mo>*</t:mo><t:mo stretchy=\"false\">)</t:mo><t:mo>+</t:mo></t:mrow></t:msup><t:mo stretchy=\"false\">(</t:mo><t:mi>u</t:mi><t:mover accent=\"true\"><t:mrow><t:mi>s</t:mi></t:mrow><t:mrow><t:mo stretchy=\"false\">¯</t:mo></t:mrow></t:mover><t:mo stretchy=\"false\">)</t:mo></t:mrow></t:math> and <hb:math xmlns:hb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><hb:mrow><hb:msup><hb:mrow><hb:mi>D</hb:mi></hb:mrow><hb:mrow><hb:mo stretchy=\"false\">(</hb:mo><hb:mo>*</hb:mo><hb:mo stretchy=\"false\">)</hb:mo><hb:mo>+</hb:mo></hb:mrow></hb:msup><hb:mo stretchy=\"false\">(</hb:mo><hb:mi>c</hb:mi><hb:mover accent=\"true\"><hb:mrow><hb:mi>d</hb:mi></hb:mrow><hb:mrow><hb:mo stretchy=\"false\">¯</hb:mo></hb:mrow></hb:mover><hb:mo stretchy=\"false\">)</hb:mo><hb:msup><hb:mrow><hb:mi>K</hb:mi></hb:mrow><hb:mrow><hb:mo stretchy=\"false\">(</hb:mo><hb:mo>*</hb:mo><hb:mo stretchy=\"false\">)</hb:mo><hb:mn>0</hb:mn></hb:mrow></hb:msup><hb:mo stretchy=\"false\">(</hb:mo><hb:mi>d</hb:mi><hb:mover accent=\"true\"><hb:mrow><hb:mi>s</hb:mi></hb:mrow><hb:mrow><hb:mo stretchy=\"false\">¯</hb:mo></hb:mrow></hb:mover><hb:mo stretchy=\"false\">)</hb:mo></hb:mrow></hb:math> rescatterings are significant. Within the commonly accepted UV cutoff range, we obtain the partial decay width <vb:math xmlns:vb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><vb:mrow><vb:mi mathvariant=\"normal\">Γ</vb:mi><vb:mo stretchy=\"false\">[</vb:mo><vb:msubsup><vb:mrow><vb:mi>D</vb:mi></vb:mrow><vb:mrow><vb:mi>s</vb:mi></vb:mrow><vb:mrow><vb:mo>*</vb:mo></vb:mrow></vb:msubsup><vb:mo stretchy=\"false\">→</vb:mo><vb:msub><vb:mrow><vb:mi>D</vb:mi></vb:mrow><vb:mrow><vb:mi>s</vb:mi></vb:mrow></vb:msub><vb:msup><vb:mrow><vb:mi>π</vb:mi></vb:mrow><vb:mrow><vb:mn>0</vb:mn></vb:mrow></vb:msup><vb:mo stretchy=\"false\">]</vb:mo><vb:mo>=</vb:mo><vb:msubsup><vb:mrow><vb:mn>9.92</vb:mn></vb:mrow><vb:mrow><vb:mo>−</vb:mo><vb:mn>0.66</vb:mn></vb:mrow><vb:mrow><vb:mo>+</vb:mo><vb:mn>0.76</vb:mn></vb:mrow></vb:msubsup><vb:mtext> </vb:mtext><vb:mtext> </vb:mtext><vb:mi>eV</vb:mi></vb:mrow></vb:math>. This approach allows us to describe the <bc:math xmlns:bc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><bc:msubsup><bc:mi>D</bc:mi><bc:mi>s</bc:mi><bc:mo>*</bc:mo></bc:msubsup></bc:math> radiative decay in the same framework via the vector-meson-dominance model. We demonstrate that both the tree-level and one-loop transitions can be self-consistently determined if we adopt the experimental data for the branching ratio fraction of <dc:math xmlns:dc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><dc:msubsup><dc:mi>D</dc:mi><dc:mi>s</dc:mi><dc:mo>*</dc:mo></dc:msubsup><dc:mo stretchy=\"false\">→</dc:mo><dc:msub><dc:mi>D</dc:mi><dc:mi>s</dc:mi></dc:msub><dc:msup><dc:mi>π</dc:mi><dc:mn>0</dc:mn></dc:msup></dc:math> to <gc:math xmlns:gc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><gc:msubsup><gc:mi>D</gc:mi><gc:mi>s</gc:mi><gc:mo>*</gc:mo></gc:msubsup><gc:mo stretchy=\"false\">→</gc:mo><gc:msub><gc:mi>D</gc:mi><gc:mi>s</gc:mi></gc:msub><gc:mi>γ</gc:mi></gc:math>. It then leads to a reliable estimate of the total decay width of <jc:math xmlns:jc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><jc:msubsup><jc:mi>D</jc:mi><jc:mi>s</jc:mi><jc:mo>*</jc:mo></jc:msubsup></jc:math>, i.e., <lc:math xmlns:lc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><lc:mrow><lc:msub><lc:mrow><lc:mi mathvariant=\"normal\">Γ</lc:mi></lc:mrow><lc:mrow><lc:mtext>total</lc:mtext></lc:mrow></lc:msub><lc:mo stretchy=\"false\">(</lc:mo><lc:msubsup><lc:mrow><lc:mi>D</lc:mi></lc:mrow><lc:mrow><lc:mi>s</lc:mi></lc:mrow><lc:mrow><lc:mo>*</lc:mo><lc:mo>+</lc:mo></lc:mrow></lc:msubsup><lc:mo stretchy=\"false\">)</lc:mo><lc:mo>=</lc:mo><lc:mn>17</lc:mn><lc:msubsup><lc:mrow><lc:mn>0</lc:mn></lc:mrow><lc:mrow><lc:mo>−</lc:mo><lc:mn>12</lc:mn></lc:mrow><lc:mrow><lc:mo>+</lc:mo><lc:mn>13</lc:mn></lc:mrow></lc:msubsup><lc:mtext> </lc:mtext><lc:mtext> </lc:mtext><lc:mi>eV</lc:mi></lc:mrow></lc:math>. <jats:supplementary-material> <jats:copyright-statement>Published by the American Physical Society</jats:copyright-statement> <jats:copyright-year>2025</jats:copyright-year> </jats:permissions> </jats:supplementary-material>","PeriodicalId":20167,"journal":{"name":"Physical Review D","volume":"25 1","pages":""},"PeriodicalIF":5.3000,"publicationDate":"2025-05-07","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Combined study of the isospin-violating decay Ds*→Dsπ0 and radiative decay Ds*→Dsγ with intermediate meson loops\",\"authors\":\"Jun Wang, Qiang Zhao\",\"doi\":\"10.1103/physrevd.111.096007\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"We carry out a combined study of the isospin-violating decay D</a:mi></a:mrow>s</a:mi></a:mrow>*</a:mo></a:mrow></a:msubsup>→</a:mo>D</a:mi></a:mrow>s</a:mi></a:mrow></a:msub>π</a:mi></a:mrow>0</a:mn></a:mrow></a:msup></a:mrow></a:math> and radiative decay <d:math xmlns:d=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><d:msubsup><d:mi>D</d:mi><d:mi>s</d:mi><d:mo>*</d:mo></d:msubsup><d:mo stretchy=\\\"false\\\">→</d:mo><d:msub><d:mi>D</d:mi><d:mi>s</d:mi></d:msub><d:mi>γ</d:mi></d:math> in an effective Lagrangian approach by taking into account the corrections from the one-loop transitions. By distinguishing the transition mechanisms of the long-distance interactions through the intermediate meson loops from the short-distance interactions through the <g:math xmlns:g=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><g:mi>η</g:mi><g:mo>−</g:mo><g:msup><g:mi>π</g:mi><g:mn>0</g:mn></g:msup></g:math> mixing at the tree level, the isospin-violating decay <i:math xmlns:i=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><i:msubsup><i:mi>D</i:mi><i:mi>s</i:mi><i:mo>*</i:mo></i:msubsup><i:mo stretchy=\\\"false\\\">→</i:mo><i:msub><i:mi>D</i:mi><i:mi>s</i:mi></i:msub><i:msup><i:mi>π</i:mi><i:mn>0</i:mn></i:msup></i:math> can be well constrained. In our approach, the higher-order corrections to the isospin-violating effects can involve the intermediate <l:math xmlns:l=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><l:msup><l:mi>D</l:mi><l:mrow><l:mo stretchy=\\\"false\\\">(</l:mo><l:mo>*</l:mo><l:mo stretchy=\\\"false\\\">)</l:mo></l:mrow></l:msup></l:math> and <p:math xmlns:p=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><p:msup><p:mi>K</p:mi><p:mrow><p:mo stretchy=\\\"false\\\">(</p:mo><p:mo>*</p:mo><p:mo stretchy=\\\"false\\\">)</p:mo></p:mrow></p:msup></p:math> scatterings. We find that the contributions from the destructive interference of intermediate meson loops via <t:math xmlns:t=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><t:mrow><t:msup><t:mrow><t:mi>D</t:mi></t:mrow><t:mrow><t:mo stretchy=\\\"false\\\">(</t:mo><t:mo>*</t:mo><t:mo stretchy=\\\"false\\\">)</t:mo><t:mn>0</t:mn></t:mrow></t:msup><t:mo stretchy=\\\"false\\\">(</t:mo><t:mi>c</t:mi><t:mover accent=\\\"true\\\"><t:mrow><t:mi>u</t:mi></t:mrow><t:mrow><t:mo stretchy=\\\"false\\\">¯</t:mo></t:mrow></t:mover><t:mo stretchy=\\\"false\\\">)</t:mo><t:msup><t:mrow><t:mi>K</t:mi></t:mrow><t:mrow><t:mo stretchy=\\\"false\\\">(</t:mo><t:mo>*</t:mo><t:mo stretchy=\\\"false\\\">)</t:mo><t:mo>+</t:mo></t:mrow></t:msup><t:mo stretchy=\\\"false\\\">(</t:mo><t:mi>u</t:mi><t:mover accent=\\\"true\\\"><t:mrow><t:mi>s</t:mi></t:mrow><t:mrow><t:mo stretchy=\\\"false\\\">¯</t:mo></t:mrow></t:mover><t:mo stretchy=\\\"false\\\">)</t:mo></t:mrow></t:math> and <hb:math xmlns:hb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><hb:mrow><hb:msup><hb:mrow><hb:mi>D</hb:mi></hb:mrow><hb:mrow><hb:mo stretchy=\\\"false\\\">(</hb:mo><hb:mo>*</hb:mo><hb:mo stretchy=\\\"false\\\">)</hb:mo><hb:mo>+</hb:mo></hb:mrow></hb:msup><hb:mo stretchy=\\\"false\\\">(</hb:mo><hb:mi>c</hb:mi><hb:mover accent=\\\"true\\\"><hb:mrow><hb:mi>d</hb:mi></hb:mrow><hb:mrow><hb:mo stretchy=\\\"false\\\">¯</hb:mo></hb:mrow></hb:mover><hb:mo stretchy=\\\"false\\\">)</hb:mo><hb:msup><hb:mrow><hb:mi>K</hb:mi></hb:mrow><hb:mrow><hb:mo stretchy=\\\"false\\\">(</hb:mo><hb:mo>*</hb:mo><hb:mo stretchy=\\\"false\\\">)</hb:mo><hb:mn>0</hb:mn></hb:mrow></hb:msup><hb:mo stretchy=\\\"false\\\">(</hb:mo><hb:mi>d</hb:mi><hb:mover accent=\\\"true\\\"><hb:mrow><hb:mi>s</hb:mi></hb:mrow><hb:mrow><hb:mo stretchy=\\\"false\\\">¯</hb:mo></hb:mrow></hb:mover><hb:mo stretchy=\\\"false\\\">)</hb:mo></hb:mrow></hb:math> rescatterings are significant. Within the commonly accepted UV cutoff range, we obtain the partial decay width <vb:math xmlns:vb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><vb:mrow><vb:mi mathvariant=\\\"normal\\\">Γ</vb:mi><vb:mo stretchy=\\\"false\\\">[</vb:mo><vb:msubsup><vb:mrow><vb:mi>D</vb:mi></vb:mrow><vb:mrow><vb:mi>s</vb:mi></vb:mrow><vb:mrow><vb:mo>*</vb:mo></vb:mrow></vb:msubsup><vb:mo stretchy=\\\"false\\\">→</vb:mo><vb:msub><vb:mrow><vb:mi>D</vb:mi></vb:mrow><vb:mrow><vb:mi>s</vb:mi></vb:mrow></vb:msub><vb:msup><vb:mrow><vb:mi>π</vb:mi></vb:mrow><vb:mrow><vb:mn>0</vb:mn></vb:mrow></vb:msup><vb:mo stretchy=\\\"false\\\">]</vb:mo><vb:mo>=</vb:mo><vb:msubsup><vb:mrow><vb:mn>9.92</vb:mn></vb:mrow><vb:mrow><vb:mo>−</vb:mo><vb:mn>0.66</vb:mn></vb:mrow><vb:mrow><vb:mo>+</vb:mo><vb:mn>0.76</vb:mn></vb:mrow></vb:msubsup><vb:mtext> </vb:mtext><vb:mtext> </vb:mtext><vb:mi>eV</vb:mi></vb:mrow></vb:math>. This approach allows us to describe the <bc:math xmlns:bc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><bc:msubsup><bc:mi>D</bc:mi><bc:mi>s</bc:mi><bc:mo>*</bc:mo></bc:msubsup></bc:math> radiative decay in the same framework via the vector-meson-dominance model. We demonstrate that both the tree-level and one-loop transitions can be self-consistently determined if we adopt the experimental data for the branching ratio fraction of <dc:math xmlns:dc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><dc:msubsup><dc:mi>D</dc:mi><dc:mi>s</dc:mi><dc:mo>*</dc:mo></dc:msubsup><dc:mo stretchy=\\\"false\\\">→</dc:mo><dc:msub><dc:mi>D</dc:mi><dc:mi>s</dc:mi></dc:msub><dc:msup><dc:mi>π</dc:mi><dc:mn>0</dc:mn></dc:msup></dc:math> to <gc:math xmlns:gc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><gc:msubsup><gc:mi>D</gc:mi><gc:mi>s</gc:mi><gc:mo>*</gc:mo></gc:msubsup><gc:mo stretchy=\\\"false\\\">→</gc:mo><gc:msub><gc:mi>D</gc:mi><gc:mi>s</gc:mi></gc:msub><gc:mi>γ</gc:mi></gc:math>. It then leads to a reliable estimate of the total decay width of <jc:math xmlns:jc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><jc:msubsup><jc:mi>D</jc:mi><jc:mi>s</jc:mi><jc:mo>*</jc:mo></jc:msubsup></jc:math>, i.e., <lc:math xmlns:lc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><lc:mrow><lc:msub><lc:mrow><lc:mi mathvariant=\\\"normal\\\">Γ</lc:mi></lc:mrow><lc:mrow><lc:mtext>total</lc:mtext></lc:mrow></lc:msub><lc:mo stretchy=\\\"false\\\">(</lc:mo><lc:msubsup><lc:mrow><lc:mi>D</lc:mi></lc:mrow><lc:mrow><lc:mi>s</lc:mi></lc:mrow><lc:mrow><lc:mo>*</lc:mo><lc:mo>+</lc:mo></lc:mrow></lc:msubsup><lc:mo stretchy=\\\"false\\\">)</lc:mo><lc:mo>=</lc:mo><lc:mn>17</lc:mn><lc:msubsup><lc:mrow><lc:mn>0</lc:mn></lc:mrow><lc:mrow><lc:mo>−</lc:mo><lc:mn>12</lc:mn></lc:mrow><lc:mrow><lc:mo>+</lc:mo><lc:mn>13</lc:mn></lc:mrow></lc:msubsup><lc:mtext> </lc:mtext><lc:mtext> </lc:mtext><lc:mi>eV</lc:mi></lc:mrow></lc:math>. <jats:supplementary-material> <jats:copyright-statement>Published by the American Physical Society</jats:copyright-statement> <jats:copyright-year>2025</jats:copyright-year> </jats:permissions> </jats:supplementary-material>\",\"PeriodicalId\":20167,\"journal\":{\"name\":\"Physical Review D\",\"volume\":\"25 1\",\"pages\":\"\"},\"PeriodicalIF\":5.3000,\"publicationDate\":\"2025-05-07\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Physical Review D\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://doi.org/10.1103/physrevd.111.096007\",\"RegionNum\":2,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q1\",\"JCRName\":\"Physics and Astronomy\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Physical Review D","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1103/physrevd.111.096007","RegionNum":2,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"Physics and Astronomy","Score":null,"Total":0}
引用次数: 0

摘要

考虑单环跃迁的修正,我们用有效的拉格朗日方法对违反同位旋的衰变Ds*→Dsπ0和辐射衰变Ds*→Dsγ进行了综合研究。通过区分通过中间介子环的远距离相互作用和通过树级η−π0混合的短距离相互作用的跃迁机制,可以很好地约束违反同位旋的衰变Ds*→Dsπ0。在我们的方法中,对同位旋违反效应的高阶修正可能涉及到中间的D(*)和K(*)散射。我们发现中间介子环通过D(*)0(cu¯)K(*)+(us¯)和D(*)+(cd¯)K(*)0(ds¯)重散射的破坏性干涉的贡献是显著的。在普遍接受的紫外截止范围内,我们得到了部分衰减宽度Γ[Ds*→Dsπ0]=9.92−0.66+0.76 eV。这种方法允许我们通过矢量-介子优势模型在相同的框架中描述Ds*辐射衰变。采用Ds*→Dsπ0到Ds*→Dsγ的分支比分数的实验数据,证明了树级跃迁和单环跃迁都是自一致的。然后得出Ds*的总衰减宽度的可靠估计,即Γtotal(Ds*+)=170−12+13 eV。2025年由美国物理学会出版
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Combined study of the isospin-violating decay Ds*→Dsπ0 and radiative decay Ds*→Dsγ with intermediate meson loops
We carry out a combined study of the isospin-violating decay Ds*→Dsπ0 and radiative decay Ds*Dsγ in an effective Lagrangian approach by taking into account the corrections from the one-loop transitions. By distinguishing the transition mechanisms of the long-distance interactions through the intermediate meson loops from the short-distance interactions through the ηπ0 mixing at the tree level, the isospin-violating decay Ds*Dsπ0 can be well constrained. In our approach, the higher-order corrections to the isospin-violating effects can involve the intermediate D(*) and K(*) scatterings. We find that the contributions from the destructive interference of intermediate meson loops via D(*)0(cu¯)K(*)+(us¯) and D(*)+(cd¯)K(*)0(ds¯) rescatterings are significant. Within the commonly accepted UV cutoff range, we obtain the partial decay width Γ[Ds*Dsπ0]=9.920.66+0.76 eV. This approach allows us to describe the Ds* radiative decay in the same framework via the vector-meson-dominance model. We demonstrate that both the tree-level and one-loop transitions can be self-consistently determined if we adopt the experimental data for the branching ratio fraction of Ds*Dsπ0 to Ds*Dsγ. It then leads to a reliable estimate of the total decay width of Ds*, i.e., Γtotal(Ds*+)=17012+13 eV. Published by the American Physical Society 2025
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来源期刊
Physical Review D
Physical Review D 物理-天文与天体物理
CiteScore
9.20
自引率
36.00%
发文量
0
审稿时长
2 months
期刊介绍: Physical Review D (PRD) is a leading journal in elementary particle physics, field theory, gravitation, and cosmology and is one of the top-cited journals in high-energy physics. PRD covers experimental and theoretical results in all aspects of particle physics, field theory, gravitation and cosmology, including: Particle physics experiments, Electroweak interactions, Strong interactions, Lattice field theories, lattice QCD, Beyond the standard model physics, Phenomenological aspects of field theory, general methods, Gravity, cosmology, cosmic rays, Astrophysics and astroparticle physics, General relativity, Formal aspects of field theory, field theory in curved space, String theory, quantum gravity, gauge/gravity duality.
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