Xiao-Dong Cheng, Zhen-Lu Weng, Ying-Ying Fan, Ru-Min Wang
{"title":"估算Bc→BK0+BK¯0→Bπ±e的CP破坏","authors":"Xiao-Dong Cheng, Zhen-Lu Weng, Ying-Ying Fan, Ru-Min Wang","doi":"10.1103/r98k-2ctc","DOIUrl":null,"url":null,"abstract":"In this paper, we investigate the C</a:mi>P</a:mi></a:math> asymmetries <c:math xmlns:c=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><c:msubsup><c:mi mathvariant=\"script\">A</c:mi><c:mrow><c:mi>C</c:mi><c:mi>P</c:mi></c:mrow><c:mrow><c:mi>p</c:mi><c:mi>m</c:mi></c:mrow></c:msubsup></c:math> and <f:math xmlns:f=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><f:msubsup><f:mi mathvariant=\"script\">A</f:mi><f:mrow><f:mi>C</f:mi><f:mi>P</f:mi></f:mrow><f:mrow><f:mi>m</f:mi><f:mi>p</f:mi></f:mrow></f:msubsup></f:math> in <i:math xmlns:i=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><i:msubsup><i:mi>B</i:mi><i:mi>c</i:mi><i:mo>±</i:mo></i:msubsup><i:mo stretchy=\"false\">→</i:mo><i:msup><i:mi>B</i:mi><i:mo>±</i:mo></i:msup><i:msup><i:mi>K</i:mi><i:mn>0</i:mn></i:msup><i:mo>+</i:mo><i:msup><i:mi>B</i:mi><i:mo>±</i:mo></i:msup><i:msup><i:mover accent=\"true\"><i:mi>K</i:mi><i:mo stretchy=\"false\">¯</i:mo></i:mover><i:mn>0</i:mn></i:msup><i:mo stretchy=\"false\">→</i:mo><i:msup><i:mi>B</i:mi><i:mo>±</i:mo></i:msup><i:msup><i:mi>π</i:mi><i:mo>±</i:mo></i:msup><i:msup><i:mi>e</i:mi><i:mo>∓</i:mo></i:msup><i:msub><i:mi>ν</i:mi><i:mi>e</i:mi></i:msub></i:math> and <o:math xmlns:o=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><o:msubsup><o:mi>B</o:mi><o:mi>c</o:mi><o:mo>±</o:mo></o:msubsup><o:mo stretchy=\"false\">→</o:mo><o:msup><o:mi>B</o:mi><o:mo>±</o:mo></o:msup><o:msup><o:mi>K</o:mi><o:mn>0</o:mn></o:msup><o:mo>+</o:mo><o:msup><o:mi>B</o:mi><o:mo>±</o:mo></o:msup><o:msup><o:mover accent=\"true\"><o:mi>K</o:mi><o:mo stretchy=\"false\">¯</o:mo></o:mover><o:mn>0</o:mn></o:msup><o:mo stretchy=\"false\">→</o:mo><o:msup><o:mi>B</o:mi><o:mo>±</o:mo></o:msup><o:msup><o:mi>π</o:mi><o:mo>∓</o:mo></o:msup><o:msup><o:mi>e</o:mi><o:mo>±</o:mo></o:msup><o:msub><o:mi>ν</o:mi><o:mi>e</o:mi></o:msub></o:math> decays; both of them consist of three parts: the indirect <u:math xmlns:u=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><u:mi>C</u:mi><u:mi>P</u:mi></u:math> violations in <w:math xmlns:w=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><w:msup><w:mi>K</w:mi><w:mn>0</w:mn></w:msup><w:mo>−</w:mo><w:msup><w:mover accent=\"true\"><w:mi>K</w:mi><w:mo stretchy=\"false\">¯</w:mo></w:mover><w:mn>0</w:mn></w:msup></w:math> mixing A</ab:mi>C</ab:mi>P</ab:mi>,</ab:mo>mix</ab:mi></ab:mrow>p</ab:mi>m</ab:mi></ab:mrow></ab:msubsup></ab:math> and <cb:math xmlns:cb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><cb:msubsup><cb:mi>A</cb:mi><cb:mrow><cb:mi>C</cb:mi><cb:mi>P</cb:mi><cb:mo>,</cb:mo><cb:mi>mix</cb:mi></cb:mrow><cb:mrow><cb:mi>m</cb:mi><cb:mi>p</cb:mi></cb:mrow></cb:msubsup></cb:math>, the direct <eb:math xmlns:eb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><eb:mi>C</eb:mi><eb:mi>P</eb:mi></eb:math> violations in <gb:math xmlns:gb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><gb:msub><gb:mi>B</gb:mi><gb:mi>c</gb:mi></gb:msub></gb:math> decay <ib:math xmlns:ib=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><ib:msubsup><ib:mi>A</ib:mi><ib:mrow><ib:mi>C</ib:mi><ib:mi>P</ib:mi><ib:mo>,</ib:mo><ib:mi>dir</ib:mi></ib:mrow><ib:mrow><ib:mi>p</ib:mi><ib:mi>m</ib:mi></ib:mrow></ib:msubsup></ib:math> and <kb:math xmlns:kb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><kb:msubsup><kb:mi>A</kb:mi><kb:mrow><kb:mi>C</kb:mi><kb:mi>P</kb:mi><kb:mo>,</kb:mo><kb:mi>dir</kb:mi></kb:mrow><kb:mrow><kb:mi>m</kb:mi><kb:mi>p</kb:mi></kb:mrow></kb:msubsup></kb:math>, and the new <mb:math xmlns:mb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mb:mi>C</mb:mi><mb:mi>P</mb:mi></mb:math> violation effects <ob:math xmlns:ob=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><ob:msubsup><ob:mi>A</ob:mi><ob:mrow><ob:mi>C</ob:mi><ob:mi>P</ob:mi><ob:mo>,</ob:mo><ob:mi>int</ob:mi></ob:mrow><ob:mrow><ob:mi>p</ob:mi><ob:mi>m</ob:mi></ob:mrow></ob:msubsup></ob:math> and <qb:math xmlns:qb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><qb:msubsup><qb:mi>A</qb:mi><qb:mrow><qb:mi>C</qb:mi><qb:mi>P</qb:mi><qb:mo>,</qb:mo><qb:mi>int</qb:mi></qb:mrow><qb:mrow><qb:mi>m</qb:mi><qb:mi>p</qb:mi></qb:mrow></qb:msubsup></qb:math>, which originate from the interference between the amplitude of the <sb:math xmlns:sb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><sb:msubsup><sb:mi>B</sb:mi><sb:mi>c</sb:mi><sb:mo>−</sb:mo></sb:msubsup><sb:mo stretchy=\"false\">→</sb:mo><sb:msup><sb:mi>B</sb:mi><sb:mo>−</sb:mo></sb:msup><sb:msup><sb:mi>K</sb:mi><sb:mn>0</sb:mn></sb:msup><sb:mo stretchy=\"false\">(</sb:mo><sb:msup><sb:mover accent=\"true\"><sb:mi>K</sb:mi><sb:mo stretchy=\"false\">¯</sb:mo></sb:mover><sb:mn>0</sb:mn></sb:msup><sb:mo stretchy=\"false\">)</sb:mo><sb:mo stretchy=\"false\">→</sb:mo><sb:msup><sb:mi>B</sb:mi><sb:mo>−</sb:mo></sb:msup><sb:msup><sb:mi>π</sb:mi><sb:mo>−</sb:mo></sb:msup><sb:msup><sb:mi>e</sb:mi><sb:mo>+</sb:mo></sb:msup><sb:msub><sb:mi>ν</sb:mi><sb:mi>e</sb:mi></sb:msub><sb:mo stretchy=\"false\">(</sb:mo><sb:msup><sb:mi>π</sb:mi><sb:mo>+</sb:mo></sb:msup><sb:msup><sb:mi>e</sb:mi><sb:mo>−</sb:mo></sb:msup><sb:msub><sb:mover accent=\"true\"><sb:mi>ν</sb:mi><sb:mo stretchy=\"false\">¯</sb:mo></sb:mover><sb:mi>e</sb:mi></sb:msub><sb:mo stretchy=\"false\">)</sb:mo></sb:math> decay with the difference between the oscillating effect of <ec:math xmlns:ec=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><ec:msup><ec:mi>K</ec:mi><ec:mn>0</ec:mn></ec:msup><ec:mo stretchy=\"false\">→</ec:mo><ec:msup><ec:mover accent=\"true\"><ec:mi>K</ec:mi><ec:mo stretchy=\"false\">¯</ec:mo></ec:mover><ec:mn>0</ec:mn></ec:msup></ec:math> and that of <jc:math xmlns:jc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><jc:msup><jc:mover accent=\"true\"><jc:mi>K</jc:mi><jc:mo stretchy=\"false\">¯</jc:mo></jc:mover><jc:mn>0</jc:mn></jc:msup><jc:mo stretchy=\"false\">→</jc:mo><jc:msup><jc:mi>K</jc:mi><jc:mn>0</jc:mn></jc:msup></jc:math>. The strong phase differences of the direct <oc:math xmlns:oc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><oc:mi>C</oc:mi><oc:mi>P</oc:mi></oc:math> asymmetries <qc:math xmlns:qc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><qc:msubsup><qc:mi>A</qc:mi><qc:mrow><qc:mi>C</qc:mi><qc:mi>P</qc:mi><qc:mo>,</qc:mo><qc:mi>dir</qc:mi></qc:mrow><qc:mrow><qc:mi>p</qc:mi><qc:mi>m</qc:mi></qc:mrow></qc:msubsup></qc:math> and <sc:math xmlns:sc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><sc:msubsup><sc:mi>A</sc:mi><sc:mrow><sc:mi>C</sc:mi><sc:mi>P</sc:mi><sc:mo>,</sc:mo><sc:mi>dir</sc:mi></sc:mrow><sc:mrow><sc:mi>m</sc:mi><sc:mi>p</sc:mi></sc:mrow></sc:msubsup></sc:math> arise from <uc:math xmlns:uc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><uc:msup><uc:mi>K</uc:mi><uc:mn>0</uc:mn></uc:msup><uc:mo>−</uc:mo><uc:msup><uc:mover accent=\"true\"><uc:mi>K</uc:mi><uc:mo stretchy=\"false\">¯</uc:mo></uc:mover><uc:mn>0</uc:mn></uc:msup></uc:math> mixing parameters. <yc:math xmlns:yc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><yc:msubsup><yc:mi mathvariant=\"script\">A</yc:mi><yc:mrow><yc:mi>C</yc:mi><yc:mi>P</yc:mi></yc:mrow><yc:mrow><yc:mi>p</yc:mi><yc:mi>m</yc:mi></yc:mrow></yc:msubsup></yc:math> and <bd:math xmlns:bd=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><bd:msubsup><bd:mi mathvariant=\"script\">A</bd:mi><bd:mrow><bd:mi>C</bd:mi><bd:mi>P</bd:mi></bd:mrow><bd:mrow><bd:mi>m</bd:mi><bd:mi>p</bd:mi></bd:mrow></bd:msubsup></bd:math> are of the order of <ed:math xmlns:ed=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><ed:mi mathvariant=\"script\">O</ed:mi><ed:mo stretchy=\"false\">(</ed:mo><ed:msup><ed:mn>10</ed:mn><ed:mrow><ed:mo>−</ed:mo><ed:mn>4</ed:mn></ed:mrow></ed:msup><ed:mo stretchy=\"false\">)</ed:mo></ed:math> and <jd:math xmlns:jd=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><jd:mi mathvariant=\"script\">O</jd:mi><jd:mo stretchy=\"false\">(</jd:mo><jd:msup><jd:mn>10</jd:mn><jd:mrow><jd:mo>−</jd:mo><jd:mn>3</jd:mn></jd:mrow></jd:msup><jd:mo stretchy=\"false\">)</jd:mo></jd:math>, respectively. The new <od:math xmlns:od=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><od:mi>C</od:mi><od:mi>P</od:mi></od:math> violation effect <qd:math xmlns:qd=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><qd:msubsup><qd:mi mathvariant=\"script\">A</qd:mi><qd:mrow><qd:mi>C</qd:mi><qd:mi>P</qd:mi><qd:mo>,</qd:mo><qd:mi>int</qd:mi></qd:mrow><qd:mrow><qd:mi>p</qd:mi><qd:mi>m</qd:mi></qd:mrow></qd:msubsup></qd:math> plays a dominant role in <td:math xmlns:td=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><td:msubsup><td:mi mathvariant=\"script\">A</td:mi><td:mrow><td:mi>C</td:mi><td:mi>P</td:mi></td:mrow><td:mrow><td:mi>p</td:mi><td:mi>m</td:mi></td:mrow></td:msubsup></td:math>; the <wd:math xmlns:wd=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><wd:mi>C</wd:mi><wd:mi>P</wd:mi></wd:math> asymmetry <yd:math xmlns:yd=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><yd:msubsup><yd:mi mathvariant=\"script\">A</yd:mi><yd:mrow><yd:mi>C</yd:mi><yd:mi>P</yd:mi></yd:mrow><yd:mrow><yd:mi>m</yd:mi><yd:mi>p</yd:mi></yd:mrow></yd:msubsup></yd:math> is dominated by the indirect <be:math xmlns:be=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><be:mi>C</be:mi><be:mi>P</be:mi></be:math> violation <de:math xmlns:de=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><de:msubsup><de:mi mathvariant=\"script\">A</de:mi><de:mrow><de:mi>C</de:mi><de:mi>P</de:mi><de:mo>,</de:mo><de:mi>mix</de:mi></de:mrow><de:mrow><de:mi>m</de:mi><de:mi>p</de:mi></de:mrow></de:msubsup></de:math>, so the <ge:math xmlns:ge=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><ge:mi>C</ge:mi><ge:mi>P</ge:mi></ge:math> asymmetry <ie:math xmlns:ie=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><ie:msubsup><ie:mi mathvariant=\"script\">A</ie:mi><ie:mrow><ie:mi>C</ie:mi><ie:mi>P</ie:mi></ie:mrow><ie:mrow><ie:mi>p</ie:mi><ie:mi>m</ie:mi></ie:mrow></ie:msubsup></ie:math> provides an ideal place to study the new <le:math xmlns:le=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><le:mi>C</le:mi><le:mi>P</le:mi></le:math> violation effect. We derive another two asymmetry observables <ne:math xmlns:ne=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><ne:msubsup><ne:mi mathvariant=\"script\">A</ne:mi><ne:mrow><ne:mi>C</ne:mi><ne:mi>P</ne:mi></ne:mrow><ne:mrow><ne:mi>p</ne:mi><ne:mi>p</ne:mi></ne:mrow></ne:msubsup></ne:math> and <qe:math xmlns:qe=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><qe:msubsup><qe:mi mathvariant=\"script\">A</qe:mi><qe:mrow><qe:mi>C</qe:mi><qe:mi>P</qe:mi></qe:mrow><qe:mrow><qe:mi>m</qe:mi><qe:mi>m</qe:mi></qe:mrow></qe:msubsup></qe:math>, which are dominated by <te:math xmlns:te=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><te:msup><te:mi>K</te:mi><te:mn>0</te:mn></te:msup><te:mo>−</te:mo><te:msup><te:mover accent=\"true\"><te:mi>K</te:mi><te:mo stretchy=\"false\">¯</te:mo></te:mover><te:mn>0</te:mn></te:msup></te:math> mixing. The observables <xe:math xmlns:xe=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><xe:msubsup><xe:mi mathvariant=\"script\">A</xe:mi><xe:mrow><xe:mi>C</xe:mi><xe:mi>P</xe:mi></xe:mrow><xe:mrow><xe:mi>p</xe:mi><xe:mi>m</xe:mi></xe:mrow></xe:msubsup></xe:math>, A</af:mi>C</af:mi>P</af:mi></af:mrow>m</af:mi>p</af:mi></af:mrow></af:msubsup></af:math>, <df:math xmlns:df=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><df:msubsup><df:mi mathvariant=\"script\">A</df:mi><df:mrow><df:mi>C</df:mi><df:mi>P</df:mi></df:mrow><df:mrow><df:mi>p</df:mi><df:mi>p</df:mi></df:mrow></df:msubsup></df:math>, and <gf:math xmlns:gf=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><gf:msubsup><gf:mi mathvariant=\"script\">A</gf:mi><gf:mrow><gf:mi>C</gf:mi><gf:mi>P</gf:mi></gf:mrow><gf:mrow><gf:mi>m</gf:mi><gf:mi>m</gf:mi></gf:mrow></gf:msubsup></gf:math> are hopefully to be marginally observed at the LHC experiment and the HL-LHC experiment.","PeriodicalId":20167,"journal":{"name":"Physical Review D","volume":"12 1","pages":""},"PeriodicalIF":5.3000,"publicationDate":"2025-10-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Estimating CP violation in Bc→BK0+BK¯0→Bπ±e∓νe decays\",\"authors\":\"Xiao-Dong Cheng, Zhen-Lu Weng, Ying-Ying Fan, Ru-Min Wang\",\"doi\":\"10.1103/r98k-2ctc\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"In this paper, we investigate the C</a:mi>P</a:mi></a:math> asymmetries <c:math xmlns:c=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><c:msubsup><c:mi mathvariant=\\\"script\\\">A</c:mi><c:mrow><c:mi>C</c:mi><c:mi>P</c:mi></c:mrow><c:mrow><c:mi>p</c:mi><c:mi>m</c:mi></c:mrow></c:msubsup></c:math> and <f:math xmlns:f=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><f:msubsup><f:mi mathvariant=\\\"script\\\">A</f:mi><f:mrow><f:mi>C</f:mi><f:mi>P</f:mi></f:mrow><f:mrow><f:mi>m</f:mi><f:mi>p</f:mi></f:mrow></f:msubsup></f:math> in <i:math xmlns:i=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><i:msubsup><i:mi>B</i:mi><i:mi>c</i:mi><i:mo>±</i:mo></i:msubsup><i:mo stretchy=\\\"false\\\">→</i:mo><i:msup><i:mi>B</i:mi><i:mo>±</i:mo></i:msup><i:msup><i:mi>K</i:mi><i:mn>0</i:mn></i:msup><i:mo>+</i:mo><i:msup><i:mi>B</i:mi><i:mo>±</i:mo></i:msup><i:msup><i:mover accent=\\\"true\\\"><i:mi>K</i:mi><i:mo stretchy=\\\"false\\\">¯</i:mo></i:mover><i:mn>0</i:mn></i:msup><i:mo stretchy=\\\"false\\\">→</i:mo><i:msup><i:mi>B</i:mi><i:mo>±</i:mo></i:msup><i:msup><i:mi>π</i:mi><i:mo>±</i:mo></i:msup><i:msup><i:mi>e</i:mi><i:mo>∓</i:mo></i:msup><i:msub><i:mi>ν</i:mi><i:mi>e</i:mi></i:msub></i:math> and <o:math xmlns:o=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><o:msubsup><o:mi>B</o:mi><o:mi>c</o:mi><o:mo>±</o:mo></o:msubsup><o:mo stretchy=\\\"false\\\">→</o:mo><o:msup><o:mi>B</o:mi><o:mo>±</o:mo></o:msup><o:msup><o:mi>K</o:mi><o:mn>0</o:mn></o:msup><o:mo>+</o:mo><o:msup><o:mi>B</o:mi><o:mo>±</o:mo></o:msup><o:msup><o:mover accent=\\\"true\\\"><o:mi>K</o:mi><o:mo stretchy=\\\"false\\\">¯</o:mo></o:mover><o:mn>0</o:mn></o:msup><o:mo stretchy=\\\"false\\\">→</o:mo><o:msup><o:mi>B</o:mi><o:mo>±</o:mo></o:msup><o:msup><o:mi>π</o:mi><o:mo>∓</o:mo></o:msup><o:msup><o:mi>e</o:mi><o:mo>±</o:mo></o:msup><o:msub><o:mi>ν</o:mi><o:mi>e</o:mi></o:msub></o:math> decays; both of them consist of three parts: the indirect <u:math xmlns:u=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><u:mi>C</u:mi><u:mi>P</u:mi></u:math> violations in <w:math xmlns:w=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><w:msup><w:mi>K</w:mi><w:mn>0</w:mn></w:msup><w:mo>−</w:mo><w:msup><w:mover accent=\\\"true\\\"><w:mi>K</w:mi><w:mo stretchy=\\\"false\\\">¯</w:mo></w:mover><w:mn>0</w:mn></w:msup></w:math> mixing A</ab:mi>C</ab:mi>P</ab:mi>,</ab:mo>mix</ab:mi></ab:mrow>p</ab:mi>m</ab:mi></ab:mrow></ab:msubsup></ab:math> and <cb:math xmlns:cb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><cb:msubsup><cb:mi>A</cb:mi><cb:mrow><cb:mi>C</cb:mi><cb:mi>P</cb:mi><cb:mo>,</cb:mo><cb:mi>mix</cb:mi></cb:mrow><cb:mrow><cb:mi>m</cb:mi><cb:mi>p</cb:mi></cb:mrow></cb:msubsup></cb:math>, the direct <eb:math xmlns:eb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><eb:mi>C</eb:mi><eb:mi>P</eb:mi></eb:math> violations in <gb:math xmlns:gb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><gb:msub><gb:mi>B</gb:mi><gb:mi>c</gb:mi></gb:msub></gb:math> decay <ib:math xmlns:ib=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><ib:msubsup><ib:mi>A</ib:mi><ib:mrow><ib:mi>C</ib:mi><ib:mi>P</ib:mi><ib:mo>,</ib:mo><ib:mi>dir</ib:mi></ib:mrow><ib:mrow><ib:mi>p</ib:mi><ib:mi>m</ib:mi></ib:mrow></ib:msubsup></ib:math> and <kb:math xmlns:kb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><kb:msubsup><kb:mi>A</kb:mi><kb:mrow><kb:mi>C</kb:mi><kb:mi>P</kb:mi><kb:mo>,</kb:mo><kb:mi>dir</kb:mi></kb:mrow><kb:mrow><kb:mi>m</kb:mi><kb:mi>p</kb:mi></kb:mrow></kb:msubsup></kb:math>, and the new <mb:math xmlns:mb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><mb:mi>C</mb:mi><mb:mi>P</mb:mi></mb:math> violation effects <ob:math xmlns:ob=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><ob:msubsup><ob:mi>A</ob:mi><ob:mrow><ob:mi>C</ob:mi><ob:mi>P</ob:mi><ob:mo>,</ob:mo><ob:mi>int</ob:mi></ob:mrow><ob:mrow><ob:mi>p</ob:mi><ob:mi>m</ob:mi></ob:mrow></ob:msubsup></ob:math> and <qb:math xmlns:qb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><qb:msubsup><qb:mi>A</qb:mi><qb:mrow><qb:mi>C</qb:mi><qb:mi>P</qb:mi><qb:mo>,</qb:mo><qb:mi>int</qb:mi></qb:mrow><qb:mrow><qb:mi>m</qb:mi><qb:mi>p</qb:mi></qb:mrow></qb:msubsup></qb:math>, which originate from the interference between the amplitude of the <sb:math xmlns:sb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><sb:msubsup><sb:mi>B</sb:mi><sb:mi>c</sb:mi><sb:mo>−</sb:mo></sb:msubsup><sb:mo stretchy=\\\"false\\\">→</sb:mo><sb:msup><sb:mi>B</sb:mi><sb:mo>−</sb:mo></sb:msup><sb:msup><sb:mi>K</sb:mi><sb:mn>0</sb:mn></sb:msup><sb:mo stretchy=\\\"false\\\">(</sb:mo><sb:msup><sb:mover accent=\\\"true\\\"><sb:mi>K</sb:mi><sb:mo stretchy=\\\"false\\\">¯</sb:mo></sb:mover><sb:mn>0</sb:mn></sb:msup><sb:mo stretchy=\\\"false\\\">)</sb:mo><sb:mo stretchy=\\\"false\\\">→</sb:mo><sb:msup><sb:mi>B</sb:mi><sb:mo>−</sb:mo></sb:msup><sb:msup><sb:mi>π</sb:mi><sb:mo>−</sb:mo></sb:msup><sb:msup><sb:mi>e</sb:mi><sb:mo>+</sb:mo></sb:msup><sb:msub><sb:mi>ν</sb:mi><sb:mi>e</sb:mi></sb:msub><sb:mo stretchy=\\\"false\\\">(</sb:mo><sb:msup><sb:mi>π</sb:mi><sb:mo>+</sb:mo></sb:msup><sb:msup><sb:mi>e</sb:mi><sb:mo>−</sb:mo></sb:msup><sb:msub><sb:mover accent=\\\"true\\\"><sb:mi>ν</sb:mi><sb:mo stretchy=\\\"false\\\">¯</sb:mo></sb:mover><sb:mi>e</sb:mi></sb:msub><sb:mo stretchy=\\\"false\\\">)</sb:mo></sb:math> decay with the difference between the oscillating effect of <ec:math xmlns:ec=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><ec:msup><ec:mi>K</ec:mi><ec:mn>0</ec:mn></ec:msup><ec:mo stretchy=\\\"false\\\">→</ec:mo><ec:msup><ec:mover accent=\\\"true\\\"><ec:mi>K</ec:mi><ec:mo stretchy=\\\"false\\\">¯</ec:mo></ec:mover><ec:mn>0</ec:mn></ec:msup></ec:math> and that of <jc:math xmlns:jc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><jc:msup><jc:mover accent=\\\"true\\\"><jc:mi>K</jc:mi><jc:mo stretchy=\\\"false\\\">¯</jc:mo></jc:mover><jc:mn>0</jc:mn></jc:msup><jc:mo stretchy=\\\"false\\\">→</jc:mo><jc:msup><jc:mi>K</jc:mi><jc:mn>0</jc:mn></jc:msup></jc:math>. The strong phase differences of the direct <oc:math xmlns:oc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><oc:mi>C</oc:mi><oc:mi>P</oc:mi></oc:math> asymmetries <qc:math xmlns:qc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><qc:msubsup><qc:mi>A</qc:mi><qc:mrow><qc:mi>C</qc:mi><qc:mi>P</qc:mi><qc:mo>,</qc:mo><qc:mi>dir</qc:mi></qc:mrow><qc:mrow><qc:mi>p</qc:mi><qc:mi>m</qc:mi></qc:mrow></qc:msubsup></qc:math> and <sc:math xmlns:sc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><sc:msubsup><sc:mi>A</sc:mi><sc:mrow><sc:mi>C</sc:mi><sc:mi>P</sc:mi><sc:mo>,</sc:mo><sc:mi>dir</sc:mi></sc:mrow><sc:mrow><sc:mi>m</sc:mi><sc:mi>p</sc:mi></sc:mrow></sc:msubsup></sc:math> arise from <uc:math xmlns:uc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><uc:msup><uc:mi>K</uc:mi><uc:mn>0</uc:mn></uc:msup><uc:mo>−</uc:mo><uc:msup><uc:mover accent=\\\"true\\\"><uc:mi>K</uc:mi><uc:mo stretchy=\\\"false\\\">¯</uc:mo></uc:mover><uc:mn>0</uc:mn></uc:msup></uc:math> mixing parameters. <yc:math xmlns:yc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><yc:msubsup><yc:mi mathvariant=\\\"script\\\">A</yc:mi><yc:mrow><yc:mi>C</yc:mi><yc:mi>P</yc:mi></yc:mrow><yc:mrow><yc:mi>p</yc:mi><yc:mi>m</yc:mi></yc:mrow></yc:msubsup></yc:math> and <bd:math xmlns:bd=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><bd:msubsup><bd:mi mathvariant=\\\"script\\\">A</bd:mi><bd:mrow><bd:mi>C</bd:mi><bd:mi>P</bd:mi></bd:mrow><bd:mrow><bd:mi>m</bd:mi><bd:mi>p</bd:mi></bd:mrow></bd:msubsup></bd:math> are of the order of <ed:math xmlns:ed=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><ed:mi mathvariant=\\\"script\\\">O</ed:mi><ed:mo stretchy=\\\"false\\\">(</ed:mo><ed:msup><ed:mn>10</ed:mn><ed:mrow><ed:mo>−</ed:mo><ed:mn>4</ed:mn></ed:mrow></ed:msup><ed:mo stretchy=\\\"false\\\">)</ed:mo></ed:math> and <jd:math xmlns:jd=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><jd:mi mathvariant=\\\"script\\\">O</jd:mi><jd:mo stretchy=\\\"false\\\">(</jd:mo><jd:msup><jd:mn>10</jd:mn><jd:mrow><jd:mo>−</jd:mo><jd:mn>3</jd:mn></jd:mrow></jd:msup><jd:mo stretchy=\\\"false\\\">)</jd:mo></jd:math>, respectively. The new <od:math xmlns:od=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><od:mi>C</od:mi><od:mi>P</od:mi></od:math> violation effect <qd:math xmlns:qd=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><qd:msubsup><qd:mi mathvariant=\\\"script\\\">A</qd:mi><qd:mrow><qd:mi>C</qd:mi><qd:mi>P</qd:mi><qd:mo>,</qd:mo><qd:mi>int</qd:mi></qd:mrow><qd:mrow><qd:mi>p</qd:mi><qd:mi>m</qd:mi></qd:mrow></qd:msubsup></qd:math> plays a dominant role in <td:math xmlns:td=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><td:msubsup><td:mi mathvariant=\\\"script\\\">A</td:mi><td:mrow><td:mi>C</td:mi><td:mi>P</td:mi></td:mrow><td:mrow><td:mi>p</td:mi><td:mi>m</td:mi></td:mrow></td:msubsup></td:math>; the <wd:math xmlns:wd=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><wd:mi>C</wd:mi><wd:mi>P</wd:mi></wd:math> asymmetry <yd:math xmlns:yd=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><yd:msubsup><yd:mi mathvariant=\\\"script\\\">A</yd:mi><yd:mrow><yd:mi>C</yd:mi><yd:mi>P</yd:mi></yd:mrow><yd:mrow><yd:mi>m</yd:mi><yd:mi>p</yd:mi></yd:mrow></yd:msubsup></yd:math> is dominated by the indirect <be:math xmlns:be=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><be:mi>C</be:mi><be:mi>P</be:mi></be:math> violation <de:math xmlns:de=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><de:msubsup><de:mi mathvariant=\\\"script\\\">A</de:mi><de:mrow><de:mi>C</de:mi><de:mi>P</de:mi><de:mo>,</de:mo><de:mi>mix</de:mi></de:mrow><de:mrow><de:mi>m</de:mi><de:mi>p</de:mi></de:mrow></de:msubsup></de:math>, so the <ge:math xmlns:ge=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><ge:mi>C</ge:mi><ge:mi>P</ge:mi></ge:math> asymmetry <ie:math xmlns:ie=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><ie:msubsup><ie:mi mathvariant=\\\"script\\\">A</ie:mi><ie:mrow><ie:mi>C</ie:mi><ie:mi>P</ie:mi></ie:mrow><ie:mrow><ie:mi>p</ie:mi><ie:mi>m</ie:mi></ie:mrow></ie:msubsup></ie:math> provides an ideal place to study the new <le:math xmlns:le=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><le:mi>C</le:mi><le:mi>P</le:mi></le:math> violation effect. We derive another two asymmetry observables <ne:math xmlns:ne=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><ne:msubsup><ne:mi mathvariant=\\\"script\\\">A</ne:mi><ne:mrow><ne:mi>C</ne:mi><ne:mi>P</ne:mi></ne:mrow><ne:mrow><ne:mi>p</ne:mi><ne:mi>p</ne:mi></ne:mrow></ne:msubsup></ne:math> and <qe:math xmlns:qe=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><qe:msubsup><qe:mi mathvariant=\\\"script\\\">A</qe:mi><qe:mrow><qe:mi>C</qe:mi><qe:mi>P</qe:mi></qe:mrow><qe:mrow><qe:mi>m</qe:mi><qe:mi>m</qe:mi></qe:mrow></qe:msubsup></qe:math>, which are dominated by <te:math xmlns:te=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><te:msup><te:mi>K</te:mi><te:mn>0</te:mn></te:msup><te:mo>−</te:mo><te:msup><te:mover accent=\\\"true\\\"><te:mi>K</te:mi><te:mo stretchy=\\\"false\\\">¯</te:mo></te:mover><te:mn>0</te:mn></te:msup></te:math> mixing. The observables <xe:math xmlns:xe=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><xe:msubsup><xe:mi mathvariant=\\\"script\\\">A</xe:mi><xe:mrow><xe:mi>C</xe:mi><xe:mi>P</xe:mi></xe:mrow><xe:mrow><xe:mi>p</xe:mi><xe:mi>m</xe:mi></xe:mrow></xe:msubsup></xe:math>, A</af:mi>C</af:mi>P</af:mi></af:mrow>m</af:mi>p</af:mi></af:mrow></af:msubsup></af:math>, <df:math xmlns:df=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><df:msubsup><df:mi mathvariant=\\\"script\\\">A</df:mi><df:mrow><df:mi>C</df:mi><df:mi>P</df:mi></df:mrow><df:mrow><df:mi>p</df:mi><df:mi>p</df:mi></df:mrow></df:msubsup></df:math>, and <gf:math xmlns:gf=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><gf:msubsup><gf:mi mathvariant=\\\"script\\\">A</gf:mi><gf:mrow><gf:mi>C</gf:mi><gf:mi>P</gf:mi></gf:mrow><gf:mrow><gf:mi>m</gf:mi><gf:mi>m</gf:mi></gf:mrow></gf:msubsup></gf:math> are hopefully to be marginally observed at the LHC experiment and the HL-LHC experiment.\",\"PeriodicalId\":20167,\"journal\":{\"name\":\"Physical Review D\",\"volume\":\"12 1\",\"pages\":\"\"},\"PeriodicalIF\":5.3000,\"publicationDate\":\"2025-10-17\",\"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/r98k-2ctc\",\"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/r98k-2ctc","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}
Estimating CP violation in Bc→BK0+BK¯0→Bπ±e∓νe decays
In this paper, we investigate the CP asymmetries ACPpm and ACPmp in Bc±→B±K0+B±K¯0→B±π±e∓νe and Bc±→B±K0+B±K¯0→B±π∓e±νe decays; both of them consist of three parts: the indirect CP violations in K0−K¯0 mixing ACP,mixpm and ACP,mixmp, the direct CP violations in Bc decay ACP,dirpm and ACP,dirmp, and the new CP violation effects ACP,intpm and ACP,intmp, which originate from the interference between the amplitude of the Bc−→B−K0(K¯0)→B−π−e+νe(π+e−ν¯e) decay with the difference between the oscillating effect of K0→K¯0 and that of K¯0→K0. The strong phase differences of the direct CP asymmetries ACP,dirpm and ACP,dirmp arise from K0−K¯0 mixing parameters. ACPpm and ACPmp are of the order of O(10−4) and O(10−3), respectively. The new CP violation effect ACP,intpm plays a dominant role in ACPpm; the CP asymmetry ACPmp is dominated by the indirect CP violation ACP,mixmp, so the CP asymmetry ACPpm provides an ideal place to study the new CP violation effect. We derive another two asymmetry observables ACPpp and ACPmm, which are dominated by K0−K¯0 mixing. The observables ACPpm, ACPmp, ACPpp, and ACPmm are hopefully to be marginally observed at the LHC experiment and the HL-LHC experiment.
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:
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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.