估算Bc→BK0+BK¯0→Bπ±e的CP破坏

IF 5.3 2区 物理与天体物理 Q1 Physics and Astronomy
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}
引用次数: 0

摘要

本文研究了Bc±→B±K0+B±K¯0→B±π±e + + + K¯0→B±π±e + + + K¯0→B±π + + + K¯0→B±π + + + K¯0→B±π + + + e±νe衰变中CP不对称性ACPpm和ACPmp;它们都由三部分组成:K0−K¯0中混合ACP、mixpm和ACP、mixmp的间接CP违背,Bc衰变中直接CP违背ACP、dirpm和ACP、dirmp,以及新的CP违背效应ACP、intpm和ACP、intmp,它们源于Bc−→B−K0(K¯0)→B−π−e+νe(π+e−ν¯e)衰减振幅之间的干扰,其振荡效应与K0→K¯0振荡效应的差异。直接CP不对称ACP,dirpm和ACP,dirmp的强相位差是由K0−K¯0混合参数引起的。ACPpm和ACPmp的数量级分别为O(10−4)和O(10−3)。新的CP违背效应ACP、intpm在ACPpm中起主导作用;CP不对称ACPmp以间接CP破坏ACP、混合ACP为主,因此CP不对称ACPpm为研究新的CP破坏效应提供了一个理想的场所。我们得到了另外两个不对称观测值ACPpp和ACPmm,它们以K0−K¯0混合为主。ACPpm、ACPmp、ACPpp和ACPmm的观测值有望在LHC实验和HL-LHC实验中边际观测到。
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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¯0B±π±eνe and Bc±B±K0+B±K¯0B±πe±νe decays; both of them consist of three parts: the indirect CP violations in K0K¯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 BcBK0(K¯0)Bπe+νe(π+eν¯e) decay with the difference between the oscillating effect of K0K¯0 and that of K¯0K0. The strong phase differences of the direct CP asymmetries ACP,dirpm and ACP,dirmp arise from K0K¯0 mixing parameters. ACPpm and ACPmp are of the order of O(104) and O(103), 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 K0K¯0 mixing. The observables ACPpm, ACPmp, ACPpp, and ACPmm are hopefully to be marginally observed at the LHC experiment and the HL-LHC experiment.
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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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