{"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><</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><</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><</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><</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}
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 B→SP 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 0.445GeV<mππ<0.795GeV. 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 Society2025
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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.
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