{"title":"夸克味道阈值在强子真空极化对μ介子反常磁矩贡献中的影响","authors":"A V Nesterenko","doi":"10.1088/1361-6471/ad0b33","DOIUrl":null,"url":null,"abstract":"The equivalent representations for the hadronic vacuum polarization contributions to the muon anomalous magnetic moment <inline-formula>\n<tex-math>\n<?CDATA ${a}_{\\mu }^{\\mathrm{HVP}}$?>\n</tex-math>\n<mml:math overflow=\"scroll\"><mml:msubsup><mml:mrow><mml:mi>a</mml:mi></mml:mrow><mml:mrow><mml:mi>μ</mml:mi></mml:mrow><mml:mrow><mml:mi>HVP</mml:mi></mml:mrow></mml:msubsup></mml:math>\n<inline-graphic xlink:href=\"jpgad0b33ieqn1.gif\" xlink:type=\"simple\"></inline-graphic>\n</inline-formula> in the presence of the quark flavour thresholds are studied. Specifically, the explicit relations between the contributions given by the integration over a finite kinematic interval to <inline-formula>\n<tex-math>\n<?CDATA ${a}_{\\mu }^{\\mathrm{HVP}}$?>\n</tex-math>\n<mml:math overflow=\"scroll\"><mml:msubsup><mml:mrow><mml:mi>a</mml:mi></mml:mrow><mml:mrow><mml:mi>μ</mml:mi></mml:mrow><mml:mrow><mml:mi>HVP</mml:mi></mml:mrow></mml:msubsup></mml:math>\n<inline-graphic xlink:href=\"jpgad0b33ieqn2.gif\" xlink:type=\"simple\"></inline-graphic>\n</inline-formula> expressed in terms of the hadronic vacuum polarization function, Adler function, and the <italic toggle=\"yes\">R</italic>-ratio of electron–positron annihilation into hadrons are derived. It is shown that the quark flavour thresholds of the hadronic vacuum polarization function generate additional contributions to <inline-formula>\n<tex-math>\n<?CDATA ${a}_{\\mu }^{\\mathrm{HVP}}$?>\n</tex-math>\n<mml:math overflow=\"scroll\"><mml:msubsup><mml:mrow><mml:mi>a</mml:mi></mml:mrow><mml:mrow><mml:mi>μ</mml:mi></mml:mrow><mml:mrow><mml:mi>HVP</mml:mi></mml:mrow></mml:msubsup></mml:math>\n<inline-graphic xlink:href=\"jpgad0b33ieqn3.gif\" xlink:type=\"simple\"></inline-graphic>\n</inline-formula> expressed in terms of the Adler function and the <italic toggle=\"yes\">R</italic>-ratio and the explicit expressions for such contributions are obtained. The commonly employed dispersion relations, which bind together hadronic vacuum polarization function, Adler function, and <italic toggle=\"yes\">R</italic>-ratio, are extended to account for the effects due to the quark flavour thresholds. The examined additional contributions due to the heavy quark thresholds to <inline-formula>\n<tex-math>\n<?CDATA ${a}_{\\mu }^{\\mathrm{HVP}}$?>\n</tex-math>\n<mml:math overflow=\"scroll\"><mml:msubsup><mml:mrow><mml:mi>a</mml:mi></mml:mrow><mml:mrow><mml:mi>μ</mml:mi></mml:mrow><mml:mrow><mml:mi>HVP</mml:mi></mml:mrow></mml:msubsup></mml:math>\n<inline-graphic xlink:href=\"jpgad0b33ieqn4.gif\" xlink:type=\"simple\"></inline-graphic>\n</inline-formula> expressed in terms of the <italic toggle=\"yes\">R</italic>-ratio appear to be quite sizable, that can be of a particular relevance for the data-driven method of assessment of the hadronic part of the muon anomalous magnetic moment.","PeriodicalId":16766,"journal":{"name":"Journal of Physics G: Nuclear and Particle Physics","volume":"12 1","pages":""},"PeriodicalIF":3.4000,"publicationDate":"2023-12-07","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Effects of the quark flavour thresholds in the hadronic vacuum polarization contributions to the muon anomalous magnetic moment\",\"authors\":\"A V Nesterenko\",\"doi\":\"10.1088/1361-6471/ad0b33\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The equivalent representations for the hadronic vacuum polarization contributions to the muon anomalous magnetic moment <inline-formula>\\n<tex-math>\\n<?CDATA ${a}_{\\\\mu }^{\\\\mathrm{HVP}}$?>\\n</tex-math>\\n<mml:math overflow=\\\"scroll\\\"><mml:msubsup><mml:mrow><mml:mi>a</mml:mi></mml:mrow><mml:mrow><mml:mi>μ</mml:mi></mml:mrow><mml:mrow><mml:mi>HVP</mml:mi></mml:mrow></mml:msubsup></mml:math>\\n<inline-graphic xlink:href=\\\"jpgad0b33ieqn1.gif\\\" xlink:type=\\\"simple\\\"></inline-graphic>\\n</inline-formula> in the presence of the quark flavour thresholds are studied. Specifically, the explicit relations between the contributions given by the integration over a finite kinematic interval to <inline-formula>\\n<tex-math>\\n<?CDATA ${a}_{\\\\mu }^{\\\\mathrm{HVP}}$?>\\n</tex-math>\\n<mml:math overflow=\\\"scroll\\\"><mml:msubsup><mml:mrow><mml:mi>a</mml:mi></mml:mrow><mml:mrow><mml:mi>μ</mml:mi></mml:mrow><mml:mrow><mml:mi>HVP</mml:mi></mml:mrow></mml:msubsup></mml:math>\\n<inline-graphic xlink:href=\\\"jpgad0b33ieqn2.gif\\\" xlink:type=\\\"simple\\\"></inline-graphic>\\n</inline-formula> expressed in terms of the hadronic vacuum polarization function, Adler function, and the <italic toggle=\\\"yes\\\">R</italic>-ratio of electron–positron annihilation into hadrons are derived. It is shown that the quark flavour thresholds of the hadronic vacuum polarization function generate additional contributions to <inline-formula>\\n<tex-math>\\n<?CDATA ${a}_{\\\\mu }^{\\\\mathrm{HVP}}$?>\\n</tex-math>\\n<mml:math overflow=\\\"scroll\\\"><mml:msubsup><mml:mrow><mml:mi>a</mml:mi></mml:mrow><mml:mrow><mml:mi>μ</mml:mi></mml:mrow><mml:mrow><mml:mi>HVP</mml:mi></mml:mrow></mml:msubsup></mml:math>\\n<inline-graphic xlink:href=\\\"jpgad0b33ieqn3.gif\\\" xlink:type=\\\"simple\\\"></inline-graphic>\\n</inline-formula> expressed in terms of the Adler function and the <italic toggle=\\\"yes\\\">R</italic>-ratio and the explicit expressions for such contributions are obtained. The commonly employed dispersion relations, which bind together hadronic vacuum polarization function, Adler function, and <italic toggle=\\\"yes\\\">R</italic>-ratio, are extended to account for the effects due to the quark flavour thresholds. The examined additional contributions due to the heavy quark thresholds to <inline-formula>\\n<tex-math>\\n<?CDATA ${a}_{\\\\mu }^{\\\\mathrm{HVP}}$?>\\n</tex-math>\\n<mml:math overflow=\\\"scroll\\\"><mml:msubsup><mml:mrow><mml:mi>a</mml:mi></mml:mrow><mml:mrow><mml:mi>μ</mml:mi></mml:mrow><mml:mrow><mml:mi>HVP</mml:mi></mml:mrow></mml:msubsup></mml:math>\\n<inline-graphic xlink:href=\\\"jpgad0b33ieqn4.gif\\\" xlink:type=\\\"simple\\\"></inline-graphic>\\n</inline-formula> expressed in terms of the <italic toggle=\\\"yes\\\">R</italic>-ratio appear to be quite sizable, that can be of a particular relevance for the data-driven method of assessment of the hadronic part of the muon anomalous magnetic moment.\",\"PeriodicalId\":16766,\"journal\":{\"name\":\"Journal of Physics G: Nuclear and Particle Physics\",\"volume\":\"12 1\",\"pages\":\"\"},\"PeriodicalIF\":3.4000,\"publicationDate\":\"2023-12-07\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Physics G: Nuclear and Particle Physics\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://doi.org/10.1088/1361-6471/ad0b33\",\"RegionNum\":3,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"PHYSICS, NUCLEAR\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Physics G: Nuclear and Particle Physics","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1088/1361-6471/ad0b33","RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"PHYSICS, NUCLEAR","Score":null,"Total":0}
引用次数: 0
摘要
研究了存在夸克味道阈值时,强子真空极化对μ介子反常磁矩aμHVP贡献的等效表示。具体地说,推导出了在有限运动学区间内对 aμHVP 的积分贡献与强子真空极化函数、阿德勒函数和电子-正电子湮灭成强子的 R 比率之间的明确关系。研究表明,强子真空极化函数的夸克味道阈值会对以阿德勒函数和 R 比率表示的 aμHVP 产生额外的贡献,并得到了这些贡献的明确表达式。常用的色散关系将强子真空极化函数、阿德勒函数和 R 比率结合在一起,并对其进行了扩展,以考虑夸克味道阈值的影响。所研究的重夸克阈值对以 R 比率表示的 aμHVP 的额外贡献似乎相当可观,这对于用数据驱动的方法评估μ介子反常磁矩的强子部分具有特别重要的意义。
Effects of the quark flavour thresholds in the hadronic vacuum polarization contributions to the muon anomalous magnetic moment
The equivalent representations for the hadronic vacuum polarization contributions to the muon anomalous magnetic moment aμHVP in the presence of the quark flavour thresholds are studied. Specifically, the explicit relations between the contributions given by the integration over a finite kinematic interval to aμHVP expressed in terms of the hadronic vacuum polarization function, Adler function, and the R-ratio of electron–positron annihilation into hadrons are derived. It is shown that the quark flavour thresholds of the hadronic vacuum polarization function generate additional contributions to aμHVP expressed in terms of the Adler function and the R-ratio and the explicit expressions for such contributions are obtained. The commonly employed dispersion relations, which bind together hadronic vacuum polarization function, Adler function, and R-ratio, are extended to account for the effects due to the quark flavour thresholds. The examined additional contributions due to the heavy quark thresholds to aμHVP expressed in terms of the R-ratio appear to be quite sizable, that can be of a particular relevance for the data-driven method of assessment of the hadronic part of the muon anomalous magnetic moment.
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