{"title":"aμ|l.ohvp, QCD power corrections and αs from e+e− → Hadrons","authors":"Stephan Narison","doi":"10.1016/j.nuclphysbps.2024.11.007","DOIUrl":null,"url":null,"abstract":"<div><div>In this talk, I review the results obtained recently in Ref. <span><span>[1]</span></span>. <em>First,</em> we estimate the LO hadronic vacuum polarization contribution to the muon and <em>τ</em> anomalous magnetic moments to be: <span><math><msub><mrow><mi>a</mi></mrow><mrow><mi>μ</mi></mrow></msub><msubsup><mrow><mo>|</mo></mrow><mrow><mi>l</mi><mo>.</mo><mi>o</mi></mrow><mrow><mi>h</mi><mi>v</mi><mi>p</mi></mrow></msubsup><mo>=</mo><mo>(</mo><mn>7036.5</mn><mo>±</mo><mn>38.9</mn><mo>)</mo><mo>×</mo><msup><mrow><mn>10</mn></mrow><mrow><mo>−</mo><mn>11</mn></mrow></msup></math></span>, <span><math><msub><mrow><mi>a</mi></mrow><mrow><mi>τ</mi></mrow></msub><msubsup><mrow><mo>|</mo></mrow><mrow><mi>l</mi><mo>.</mo><mi>o</mi></mrow><mrow><mi>h</mi><mi>v</mi><mi>p</mi></mrow></msubsup><mo>=</mo><mo>(</mo><mn>3494.8</mn><mo>±</mo><mn>24.7</mn><mo>)</mo><mo>×</mo><msup><mrow><mn>10</mn></mrow><mrow><mo>−</mo><mn>9</mn></mrow></msup></math></span> (see Table 1) leading to: <span><math><mi>Δ</mi><msub><mrow><mi>a</mi></mrow><mrow><mi>μ</mi></mrow></msub><mo>≡</mo><msubsup><mrow><mi>a</mi></mrow><mrow><mi>μ</mi></mrow><mrow><mi>e</mi><mi>x</mi><mi>p</mi></mrow></msubsup><mo>−</mo><msubsup><mrow><mi>a</mi></mrow><mrow><mi>μ</mi></mrow><mrow><mi>S</mi><mi>M</mi></mrow></msubsup><mo>=</mo><mo>(</mo><mn>143</mn><mo>±</mo><msub><mrow><mn>42</mn></mrow><mrow><mi>t</mi><mi>h</mi></mrow></msub><mo>±</mo><msub><mrow><mn>22</mn></mrow><mrow><mi>e</mi><mi>x</mi><mi>p</mi></mrow></msub><mo>)</mo><mo>×</mo><msup><mrow><mn>10</mn></mrow><mrow><mo>−</mo><mn>11</mn></mrow></msup></math></span> which is about 3<em>σ</em> discrepancy between the SM predictions and experiment. One also finds: <span><math><msup><mrow><mi>α</mi></mrow><mrow><mo>(</mo><mn>5</mn><mo>)</mo></mrow></msup><mo>(</mo><msub><mrow><mi>M</mi></mrow><mrow><mi>Z</mi></mrow></msub><mo>)</mo><msub><mrow><mo>|</mo></mrow><mrow><mi>h</mi><mi>a</mi><mi>d</mi></mrow></msub><mo>=</mo><mo>(</mo><mn>2766.3</mn><mo>±</mo><mn>4.5</mn><mo>)</mo><mo>×</mo><msup><mrow><mn>10</mn></mrow><mrow><mo>−</mo><mn>5</mn></mrow></msup></math></span>. <em>Second,</em> we estimate the QCD power corrections up to dimension 20 from the ratio of Laplace sum rule and from <em>τ</em>-like decay high moments (see Table 3). We do not observe any exponential growth of their size which may not favour a duality violation of the spectral function. We obtain <span><math><mo>〈</mo><msub><mrow><mi>α</mi></mrow><mrow><mi>s</mi></mrow></msub><msup><mrow><mi>G</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>〉</mo><mo>=</mo><mo>(</mo><mn>7.8</mn><mo>±</mo><mn>3.5</mn><mo>)</mo><mo>×</mo><msup><mrow><mn>10</mn></mrow><mrow><mo>−</mo><mn>2</mn></mrow></msup><mspace></mspace><msup><mrow><mtext>GeV</mtext></mrow><mrow><mn>4</mn></mrow></msup></math></span> in agreement with the more precise one from heavy quark sum rules, while <span><math><mi>ρ</mi><msub><mrow><mi>α</mi></mrow><mrow><mi>s</mi></mrow></msub><msup><mrow><mo>〈</mo><mover><mrow><mi>ψ</mi></mrow><mrow><mo>¯</mo></mrow></mover><mi>ψ</mi><mo>〉</mo></mrow><mrow><mn>2</mn></mrow></msup><mo>=</mo><mo>(</mo><mn>5.98</mn><mo>±</mo><mn>0.64</mn><mo>)</mo><mo>×</mo><msup><mrow><mn>10</mn></mrow><mrow><mo>−</mo><mn>4</mn></mrow></msup><mspace></mspace><msup><mrow><mtext>GeV</mtext></mrow><mrow><mn>6</mn></mrow></msup></math></span> confirms a violation of the four-quark condensate factorization by a factor <span><math><mi>ρ</mi><mo>≃</mo><mn>6</mn></math></span>. <em>Third</em>, using the previous values of the condensates, we re-extract <span><math><msub><mrow><mi>α</mi></mrow><mrow><mi>s</mi></mrow></msub></math></span> from the lowest <em>τ</em>-decay Braaten-SN-Pich (BNP) moment and find to order <span><math><msubsup><mrow><mi>α</mi></mrow><mrow><mi>s</mi></mrow><mrow><mn>4</mn></mrow></msubsup><mo>:</mo><msub><mrow><mi>α</mi></mrow><mrow><mi>s</mi></mrow></msub><mo>(</mo><msub><mrow><mi>M</mi></mrow><mrow><mi>τ</mi></mrow></msub><mo>)</mo><mo>=</mo><mn>0.3081</mn><mo>(</mo><mn>86</mn><mo>)</mo><mspace></mspace><mo>[</mo><mrow><mi>resp</mi><mo>.</mo></mrow><mspace></mspace><mn>0.3260</mn><mo>(</mo><mn>79</mn><mo>)</mo><mo>]</mo><mo>⟶</mo><mspace></mspace><mo>∘</mo><mspace></mspace><mspace></mspace><msub><mrow><mi>α</mi></mrow><mrow><mi>s</mi></mrow></msub><mo>(</mo><msub><mrow><mi>M</mi></mrow><mrow><mi>Z</mi></mrow></msub><mo>)</mo><mo>=</mo><mn>0.1170</mn><mo>(</mo><mn>7</mn><mo>)</mo><mspace></mspace><mo>[</mo><mrow><mi>resp</mi><mo>.</mo></mrow><mspace></mspace><mn>0.1192</mn><mo>(</mo><mn>7</mn><mo>)</mo><mo>]</mo></math></span> for Fixed Order (FO) [resp. Contour Improved (CI)] PT series. We also show that the contributions beyond the Shifman-Vainshtein-Zakharov (SVZ)-expansion are negligible.</div></div>","PeriodicalId":37968,"journal":{"name":"Nuclear and Particle Physics Proceedings","volume":"347 ","pages":"Pages 105-115"},"PeriodicalIF":0.0000,"publicationDate":"2024-12-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Nuclear and Particle Physics Proceedings","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S2405601424001718","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q4","JCRName":"Physics and Astronomy","Score":null,"Total":0}
引用次数: 0
Abstract
In this talk, I review the results obtained recently in Ref. [1]. First, we estimate the LO hadronic vacuum polarization contribution to the muon and τ anomalous magnetic moments to be: , (see Table 1) leading to: which is about 3σ discrepancy between the SM predictions and experiment. One also finds: . Second, we estimate the QCD power corrections up to dimension 20 from the ratio of Laplace sum rule and from τ-like decay high moments (see Table 3). We do not observe any exponential growth of their size which may not favour a duality violation of the spectral function. We obtain in agreement with the more precise one from heavy quark sum rules, while confirms a violation of the four-quark condensate factorization by a factor . Third, using the previous values of the condensates, we re-extract from the lowest τ-decay Braaten-SN-Pich (BNP) moment and find to order for Fixed Order (FO) [resp. Contour Improved (CI)] PT series. We also show that the contributions beyond the Shifman-Vainshtein-Zakharov (SVZ)-expansion are negligible.
期刊介绍:
Nuclear and Particle Physics Proceedings is the premier publication outlet for the proceedings of key conferences on nuclear and high-energy physics and related areas. The series covers both large international conferences and topical meetings. The newest discoveries and the latest developments, reported at carefully selected meetings, are published covering experimental as well as theoretical particle physics, nuclear and hadronic physics, cosmology, astrophysics and gravitation, field theory and statistical systems, and physical mathematics.