用QCD分解法探测涉及标量介子的B衰变中的软重散射参数

IF 5.3 2区 物理与天体物理 Q1 Physics and Astronomy
Jing-Juan Qi, Zhen-Yang Wang, Zhen-Hua Zhang, Ke-Wei Wei, Xin-Heng Guo
{"title":"用QCD分解法探测涉及标量介子的B衰变中的软重散射参数","authors":"Jing-Juan Qi, Zhen-Yang Wang, Zhen-Hua Zhang, Ke-Wei Wei, Xin-Heng Guo","doi":"10.1103/physrevd.111.016017","DOIUrl":null,"url":null,"abstract":"In this work, the soft rescattering parameters in the B</a:mi>±</a:mo></a:msup>→</a:mo>π</a:mi>±</a:mo></a:msup>π</a:mi>+</a:mo></a:msup>π</a:mi>−</a:mo></a:msup></a:math> and <d:math xmlns:d=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><d:msup><d:mi>B</d:mi><d:mo>±</d:mo></d:msup><d:mo stretchy=\"false\">→</d:mo><d:msup><d:mi>K</d:mi><d:mo>±</d:mo></d:msup><d:msup><d:mi>π</d:mi><d:mo>+</d:mo></d:msup><d:msup><d:mi>π</d:mi><d:mo>−</d:mo></d:msup></d:math> decays with the light scalar meson <g:math xmlns:g=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><g:msub><g:mi>f</g:mi><g:mn>0</g:mn></g:msub><g:mo stretchy=\"false\">(</g:mo><g:mn>500</g:mn><g:mo stretchy=\"false\">)</g:mo></g:math> as the intermediate resonance are studied within the quantum chromodynamics (QCD) factorization. Considering the interference effect between <k:math xmlns:k=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><k:mi>ρ</k:mi><k:mo stretchy=\"false\">(</k:mo><k:mn>770</k:mn><k:msup><k:mo stretchy=\"false\">)</k:mo><k:mn>0</k:mn></k:msup></k:math> and <o:math xmlns:o=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><o:msub><o:mi>f</o:mi><o:mn>0</o:mn></o:msub><o:mo stretchy=\"false\">(</o:mo><o:mn>500</o:mn><o:mo stretchy=\"false\">)</o:mo></o:math>, we utilize the experimentally more direct event yields for fitting and get the soft rescattering parameters <s:math xmlns:s=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><s:mo stretchy=\"false\">|</s:mo><s:msubsup><s:mi>ρ</s:mi><s:mi>k</s:mi><s:mrow><s:mi>S</s:mi><s:mi>P</s:mi></s:mrow></s:msubsup><s:mo stretchy=\"false\">|</s:mo><s:mo>=</s:mo><s:mn>3.29</s:mn><s:mo>±</s:mo><s:mn>1.01</s:mn></s:math> and <w:math xmlns:w=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><w:mo stretchy=\"false\">|</w:mo><w:msubsup><w:mi>ρ</w:mi><w:mi>k</w:mi><w:mrow><w:mi>P</w:mi><w:mi>S</w:mi></w:mrow></w:msubsup><w:mo stretchy=\"false\">|</w:mo><w:mo>=</w:mo><w:mn>2.33</w:mn><w:mo>±</w:mo><w:mn>0.73</w:mn></w:math> in B</ab:mi>→</ab:mo>P</ab:mi>S</ab:mi></ab:math> and <db:math xmlns:db=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><db:mi>B</db:mi><db:mo stretchy=\"false\">→</db:mo><db:mi>S</db:mi><db:mi>P</db:mi></db:math> decays (<gb:math xmlns:gb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><gb:mi>P</gb:mi></gb:math> and <ib:math xmlns:ib=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><ib:mi>S</ib:mi></ib:math> denote pseudoscalar and scalar mesons, respectively), respectively. We also study the branching ratios and <kb:math xmlns:kb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><kb:mi>C</kb:mi><kb:mi>P</kb:mi></kb:math> asymmetries in the decay modes involving other scalar mesons, including <mb:math xmlns:mb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mb:msub><mb:mi>f</mb:mi><mb:mn>0</mb:mn></mb:msub><mb:mo stretchy=\"false\">(</mb:mo><mb:mn>980</mb:mn><mb:mo stretchy=\"false\">)</mb:mo></mb:math>, <qb:math xmlns:qb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><qb:msub><qb:mi>a</qb:mi><qb:mn>0</qb:mn></qb:msub><qb:mo stretchy=\"false\">(</qb:mo><qb:mn>980</qb:mn><qb:mo stretchy=\"false\">)</qb:mo></qb:math>, <ub:math xmlns:ub=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><ub:msub><ub:mi>a</ub:mi><ub:mn>0</ub:mn></ub:msub><ub:mo stretchy=\"false\">(</ub:mo><ub:mn>1450</ub:mn><ub:mo stretchy=\"false\">)</ub:mo></ub:math> and <yb:math xmlns:yb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><yb:msubsup><yb:mi>K</yb:mi><yb:mn>0</yb:mn><yb:mo>*</yb:mo></yb:msubsup><yb:mo stretchy=\"false\">(</yb:mo><yb:mn>1430</yb:mn><yb:mo stretchy=\"false\">)</yb:mo></yb:math>, to test the rationality of the values of <cc:math xmlns:cc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><cc:mo stretchy=\"false\">|</cc:mo><cc:msubsup><cc:mi>ρ</cc:mi><cc:mi>k</cc:mi><cc:mrow><cc:mi>S</cc:mi><cc:mi>P</cc:mi></cc:mrow></cc:msubsup><cc:mo stretchy=\"false\">|</cc:mo></cc:math> and <gc:math xmlns:gc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><gc:mo stretchy=\"false\">|</gc:mo><gc:msubsup><gc:mi>ρ</gc:mi><gc:mi>k</gc:mi><gc:mrow><gc:mi>P</gc:mi><gc:mi>S</gc:mi></gc:mrow></gc:msubsup><gc:mo stretchy=\"false\">|</gc:mo></gc:math>. Meanwhile, the wealth of experimental data facilitate the examination of the forward-backward asymmetry induced <kc:math xmlns:kc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><kc:mi>C</kc:mi><kc:mi>P</kc:mi></kc:math> asymmetries (FB-CPAs), and the localized <mc:math xmlns:mc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mc:mi>C</mc:mi><mc:mi>P</mc:mi></mc:math> asymmetries (LACPs). We investigate these asymmetries resulting from the interference between <oc:math xmlns:oc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><oc:mi>ρ</oc:mi><oc:mo stretchy=\"false\">(</oc:mo><oc:mn>770</oc:mn><oc:msup><oc:mo stretchy=\"false\">)</oc:mo><oc:mn>0</oc:mn></oc:msup></oc:math> and <sc:math xmlns:sc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><sc:msub><sc:mi>f</sc:mi><sc:mn>0</sc:mn></sc:msub><sc:mo stretchy=\"false\">(</sc:mo><sc:mn>500</sc:mn><sc:mo stretchy=\"false\">)</sc:mo></sc:math> for <wc:math xmlns:wc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><wc:msup><wc:mi>B</wc:mi><wc:mo>±</wc:mo></wc:msup><wc:mo stretchy=\"false\">→</wc:mo><wc:msup><wc:mi>π</wc:mi><wc:mo>±</wc:mo></wc:msup><wc:msup><wc:mi>π</wc:mi><wc:mo>+</wc:mo></wc:msup><wc:msup><wc:mi>π</wc:mi><wc:mo>−</wc:mo></wc:msup></wc:math> and <zc:math xmlns:zc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><zc:msup><zc:mi>B</zc:mi><zc:mo>±</zc:mo></zc:msup><zc:mo stretchy=\"false\">→</zc:mo><zc:msup><zc:mi>K</zc:mi><zc:mo>±</zc:mo></zc:msup><zc:msup><zc:mi>π</zc:mi><zc:mo>+</zc:mo></zc:msup><zc:msup><zc:mi>π</zc:mi><zc:mo>−</zc:mo></zc:msup></zc:math> decays when the invariant mass of <cd:math xmlns:cd=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><cd:msup><cd:mi>π</cd:mi><cd:mo>+</cd:mo></cd:msup><cd:msup><cd:mi>π</cd:mi><cd:mo>−</cd:mo></cd:msup></cd:math> locates in the low-energy region <ed:math xmlns:ed=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><ed:mn>0.445</ed:mn><ed:mtext> </ed:mtext><ed:mtext> </ed:mtext><ed:mi>GeV</ed:mi><ed:mo>&lt;</ed:mo><ed:msub><ed:mi>m</ed:mi><ed:mrow><ed:mi>π</ed:mi><ed:mi>π</ed:mi></ed:mrow></ed:msub><ed:mo>&lt;</ed:mo><ed:mn>0.795</ed:mn><ed:mtext> </ed:mtext><ed:mtext> </ed:mtext><ed:mi>GeV</ed:mi></ed:math>. Our theoretical results of FB-CPAs and LACPs align with the experimental findings. We propose that the interference between <gd:math xmlns:gd=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><gd:mi>ρ</gd:mi><gd:mo stretchy=\"false\">(</gd:mo><gd:mn>770</gd:mn><gd:msup><gd:mo stretchy=\"false\">)</gd:mo><gd:mn>0</gd:mn></gd:msup></gd:math> and <kd:math xmlns:kd=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><kd:msub><kd:mi>f</kd:mi><kd:mn>0</kd:mn></kd:msub><kd:mo stretchy=\"false\">(</kd:mo><kd:mn>500</kd:mn><kd:mo stretchy=\"false\">)</kd:mo></kd:math> can be extended to other beauty and charmed mesons decays. <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":"27 1","pages":""},"PeriodicalIF":5.3000,"publicationDate":"2025-01-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Probing the soft rescattering parameters in B decays involving a scalar meson with QCD factorization\",\"authors\":\"Jing-Juan Qi, Zhen-Yang Wang, Zhen-Hua Zhang, Ke-Wei Wei, Xin-Heng Guo\",\"doi\":\"10.1103/physrevd.111.016017\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"In this work, the soft rescattering parameters in the B</a:mi>±</a:mo></a:msup>→</a:mo>π</a:mi>±</a:mo></a:msup>π</a:mi>+</a:mo></a:msup>π</a:mi>−</a:mo></a:msup></a:math> and <d:math xmlns:d=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><d:msup><d:mi>B</d:mi><d:mo>±</d:mo></d:msup><d:mo stretchy=\\\"false\\\">→</d:mo><d:msup><d:mi>K</d:mi><d:mo>±</d:mo></d:msup><d:msup><d:mi>π</d:mi><d:mo>+</d:mo></d:msup><d:msup><d:mi>π</d:mi><d:mo>−</d:mo></d:msup></d:math> decays with the light scalar meson <g:math xmlns:g=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><g:msub><g:mi>f</g:mi><g:mn>0</g:mn></g:msub><g:mo stretchy=\\\"false\\\">(</g:mo><g:mn>500</g:mn><g:mo stretchy=\\\"false\\\">)</g:mo></g:math> as the intermediate resonance are studied within the quantum chromodynamics (QCD) factorization. Considering the interference effect between <k:math xmlns:k=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><k:mi>ρ</k:mi><k:mo stretchy=\\\"false\\\">(</k:mo><k:mn>770</k:mn><k:msup><k:mo stretchy=\\\"false\\\">)</k:mo><k:mn>0</k:mn></k:msup></k:math> and <o:math xmlns:o=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><o:msub><o:mi>f</o:mi><o:mn>0</o:mn></o:msub><o:mo stretchy=\\\"false\\\">(</o:mo><o:mn>500</o:mn><o:mo stretchy=\\\"false\\\">)</o:mo></o:math>, we utilize the experimentally more direct event yields for fitting and get the soft rescattering parameters <s:math xmlns:s=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><s:mo stretchy=\\\"false\\\">|</s:mo><s:msubsup><s:mi>ρ</s:mi><s:mi>k</s:mi><s:mrow><s:mi>S</s:mi><s:mi>P</s:mi></s:mrow></s:msubsup><s:mo stretchy=\\\"false\\\">|</s:mo><s:mo>=</s:mo><s:mn>3.29</s:mn><s:mo>±</s:mo><s:mn>1.01</s:mn></s:math> and <w:math xmlns:w=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><w:mo stretchy=\\\"false\\\">|</w:mo><w:msubsup><w:mi>ρ</w:mi><w:mi>k</w:mi><w:mrow><w:mi>P</w:mi><w:mi>S</w:mi></w:mrow></w:msubsup><w:mo stretchy=\\\"false\\\">|</w:mo><w:mo>=</w:mo><w:mn>2.33</w:mn><w:mo>±</w:mo><w:mn>0.73</w:mn></w:math> in B</ab:mi>→</ab:mo>P</ab:mi>S</ab:mi></ab:math> and <db:math xmlns:db=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><db:mi>B</db:mi><db:mo stretchy=\\\"false\\\">→</db:mo><db:mi>S</db:mi><db:mi>P</db:mi></db:math> decays (<gb:math xmlns:gb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><gb:mi>P</gb:mi></gb:math> and <ib:math xmlns:ib=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><ib:mi>S</ib:mi></ib:math> denote pseudoscalar and scalar mesons, respectively), respectively. We also study the branching ratios and <kb:math xmlns:kb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><kb:mi>C</kb:mi><kb:mi>P</kb:mi></kb:math> asymmetries in the decay modes involving other scalar mesons, including <mb:math xmlns:mb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><mb:msub><mb:mi>f</mb:mi><mb:mn>0</mb:mn></mb:msub><mb:mo stretchy=\\\"false\\\">(</mb:mo><mb:mn>980</mb:mn><mb:mo stretchy=\\\"false\\\">)</mb:mo></mb:math>, <qb:math xmlns:qb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><qb:msub><qb:mi>a</qb:mi><qb:mn>0</qb:mn></qb:msub><qb:mo stretchy=\\\"false\\\">(</qb:mo><qb:mn>980</qb:mn><qb:mo stretchy=\\\"false\\\">)</qb:mo></qb:math>, <ub:math xmlns:ub=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><ub:msub><ub:mi>a</ub:mi><ub:mn>0</ub:mn></ub:msub><ub:mo stretchy=\\\"false\\\">(</ub:mo><ub:mn>1450</ub:mn><ub:mo stretchy=\\\"false\\\">)</ub:mo></ub:math> and <yb:math xmlns:yb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><yb:msubsup><yb:mi>K</yb:mi><yb:mn>0</yb:mn><yb:mo>*</yb:mo></yb:msubsup><yb:mo stretchy=\\\"false\\\">(</yb:mo><yb:mn>1430</yb:mn><yb:mo stretchy=\\\"false\\\">)</yb:mo></yb:math>, to test the rationality of the values of <cc:math xmlns:cc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><cc:mo stretchy=\\\"false\\\">|</cc:mo><cc:msubsup><cc:mi>ρ</cc:mi><cc:mi>k</cc:mi><cc:mrow><cc:mi>S</cc:mi><cc:mi>P</cc:mi></cc:mrow></cc:msubsup><cc:mo stretchy=\\\"false\\\">|</cc:mo></cc:math> and <gc:math xmlns:gc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><gc:mo stretchy=\\\"false\\\">|</gc:mo><gc:msubsup><gc:mi>ρ</gc:mi><gc:mi>k</gc:mi><gc:mrow><gc:mi>P</gc:mi><gc:mi>S</gc:mi></gc:mrow></gc:msubsup><gc:mo stretchy=\\\"false\\\">|</gc:mo></gc:math>. Meanwhile, the wealth of experimental data facilitate the examination of the forward-backward asymmetry induced <kc:math xmlns:kc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><kc:mi>C</kc:mi><kc:mi>P</kc:mi></kc:math> asymmetries (FB-CPAs), and the localized <mc:math xmlns:mc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><mc:mi>C</mc:mi><mc:mi>P</mc:mi></mc:math> asymmetries (LACPs). We investigate these asymmetries resulting from the interference between <oc:math xmlns:oc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><oc:mi>ρ</oc:mi><oc:mo stretchy=\\\"false\\\">(</oc:mo><oc:mn>770</oc:mn><oc:msup><oc:mo stretchy=\\\"false\\\">)</oc:mo><oc:mn>0</oc:mn></oc:msup></oc:math> and <sc:math xmlns:sc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><sc:msub><sc:mi>f</sc:mi><sc:mn>0</sc:mn></sc:msub><sc:mo stretchy=\\\"false\\\">(</sc:mo><sc:mn>500</sc:mn><sc:mo stretchy=\\\"false\\\">)</sc:mo></sc:math> for <wc:math xmlns:wc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><wc:msup><wc:mi>B</wc:mi><wc:mo>±</wc:mo></wc:msup><wc:mo stretchy=\\\"false\\\">→</wc:mo><wc:msup><wc:mi>π</wc:mi><wc:mo>±</wc:mo></wc:msup><wc:msup><wc:mi>π</wc:mi><wc:mo>+</wc:mo></wc:msup><wc:msup><wc:mi>π</wc:mi><wc:mo>−</wc:mo></wc:msup></wc:math> and <zc:math xmlns:zc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><zc:msup><zc:mi>B</zc:mi><zc:mo>±</zc:mo></zc:msup><zc:mo stretchy=\\\"false\\\">→</zc:mo><zc:msup><zc:mi>K</zc:mi><zc:mo>±</zc:mo></zc:msup><zc:msup><zc:mi>π</zc:mi><zc:mo>+</zc:mo></zc:msup><zc:msup><zc:mi>π</zc:mi><zc:mo>−</zc:mo></zc:msup></zc:math> decays when the invariant mass of <cd:math xmlns:cd=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><cd:msup><cd:mi>π</cd:mi><cd:mo>+</cd:mo></cd:msup><cd:msup><cd:mi>π</cd:mi><cd:mo>−</cd:mo></cd:msup></cd:math> locates in the low-energy region <ed:math xmlns:ed=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><ed:mn>0.445</ed:mn><ed:mtext> </ed:mtext><ed:mtext> </ed:mtext><ed:mi>GeV</ed:mi><ed:mo>&lt;</ed:mo><ed:msub><ed:mi>m</ed:mi><ed:mrow><ed:mi>π</ed:mi><ed:mi>π</ed:mi></ed:mrow></ed:msub><ed:mo>&lt;</ed:mo><ed:mn>0.795</ed:mn><ed:mtext> </ed:mtext><ed:mtext> </ed:mtext><ed:mi>GeV</ed:mi></ed:math>. Our theoretical results of FB-CPAs and LACPs align with the experimental findings. We propose that the interference between <gd:math xmlns:gd=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><gd:mi>ρ</gd:mi><gd:mo stretchy=\\\"false\\\">(</gd:mo><gd:mn>770</gd:mn><gd:msup><gd:mo stretchy=\\\"false\\\">)</gd:mo><gd:mn>0</gd:mn></gd:msup></gd:math> and <kd:math xmlns:kd=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><kd:msub><kd:mi>f</kd:mi><kd:mn>0</kd:mn></kd:msub><kd:mo stretchy=\\\"false\\\">(</kd:mo><kd:mn>500</kd:mn><kd:mo stretchy=\\\"false\\\">)</kd:mo></kd:math> can be extended to other beauty and charmed mesons decays. <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\":\"27 1\",\"pages\":\"\"},\"PeriodicalIF\":5.3000,\"publicationDate\":\"2025-01-14\",\"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.111.016017\",\"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.111.016017","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

本文在量子色动力学(QCD)因子化中研究了以轻标量介子f0(500)为中间共振的B±→π±π+π-和B±→K±π+π-衰变中的软反散射参数。考虑到ρ(770)0和f0(500)之间的干涉效应,我们利用实验中更直接的事件产率进行拟合,得到了B→PS和B→SP衰变(P和S分别表示伪标量介子和标量介子)中的软散射参数|ρkSP|=3.29±1.01和|ρkPS|=2.33±0.73。我们还研究了其他标量介子衰变模式的分支比和CP不对称,包括f0(980)、a0(980)、a0(1450)和K0*(1430),以检验|ρkSP|和|ρkPS|值的合理性。同时,丰富的实验数据也为检验前后不对称诱导的CP不对称(FB-CPAs)和局部CP不对称(LACPs)提供了便利。当π+π-的不变质量位于0.445 GeV<mππ<0.795 GeV的低能区时,我们研究了B±→π±π+π-和B±→K±π+π-衰变的ρ(770)0和f0(500)之间的干涉导致的这些不对称。我们的 FB-CPAs 和 LACPs 理论结果与实验结果一致。我们提出,ρ(770)0和f0(500)之间的干涉可以扩展到其他美介子和粲介子衰变。 美国物理学会出版 2025
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Probing the soft rescattering parameters in B decays involving a scalar meson with QCD factorization
In this work, the soft rescattering parameters in the B±→π±π+π− and B±K±π+π decays with the light scalar meson f0(500) as the intermediate resonance are studied within the quantum chromodynamics (QCD) factorization. Considering the interference effect between ρ(770)0 and f0(500), we utilize the experimentally more direct event yields for fitting and get the soft rescattering parameters |ρkSP|=3.29±1.01 and |ρkPS|=2.33±0.73 in B→PS and BSP decays (P and S denote pseudoscalar and scalar mesons, respectively), respectively. We also study the branching ratios and CP asymmetries in the decay modes involving other scalar mesons, including f0(980), a0(980), a0(1450) and K0*(1430), to test the rationality of the values of |ρkSP| and |ρkPS|. Meanwhile, the wealth of experimental data facilitate the examination of the forward-backward asymmetry induced CP asymmetries (FB-CPAs), and the localized CP asymmetries (LACPs). We investigate these asymmetries resulting from the interference between ρ(770)0 and f0(500) for B±π±π+π and B±K±π+π decays when the invariant mass of π+π locates in the low-energy region 0.445 GeV<mππ<0.795 GeV. Our theoretical results of FB-CPAs and LACPs align with the experimental findings. We propose that the interference between ρ(770)0 and f0(500) can be extended to other beauty and charmed mesons decays. 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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