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$\alpha_s$ and |$\rm V_{cs}$| determination, and CKM unitarity test, from W decays at NNLO
The hadronic ($\Gamma^{\rm W}_{\rm had}$) and total ($\Gamma^{\rm W}_{\rm tot}$) widths of the W boson, computed at least at next-to-next-to-leading-order (NNLO) accuracy, are combined to derive a new precise prediction for the hadronic W branching ratio ${\cal B}^{\rm W}_{\rm had} \equiv \Gamma^{\r...
Autores principales: | , |
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Lenguaje: | eng |
Publicado: |
2016
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Acceso en línea: | https://dx.doi.org/10.1016/j.physletb.2016.10.012 http://cds.cern.ch/record/2140736 |
_version_ | 1780950096061399040 |
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author | d'Enterria, David Srebre, Matej |
author_facet | d'Enterria, David Srebre, Matej |
author_sort | d'Enterria, David |
collection | CERN |
description | The hadronic ($\Gamma^{\rm W}_{\rm had}$) and total ($\Gamma^{\rm W}_{\rm tot}$) widths of the W boson, computed at least at next-to-next-to-leading-order (NNLO) accuracy, are combined to derive a new precise prediction for the hadronic W branching ratio ${\cal B}^{\rm W}_{\rm had} \equiv \Gamma^{\rm W}_{\rm had}/\Gamma^{\rm W}_{\rm tot}$ = $0.682 \pm 0.011_{\rm par}$, using the experimental Cabibbo-Kobayashi-Maskawa (CKM) matrix elements, or ${\cal B}^{\rm W}_{\rm had} = 0.6742 \pm 0.0002_{\rm th} \pm 0.0001_{\rm par}$ assuming CKM unitarity, with uncertainties dominated by the input parameters of the calculations. Comparing the theoretical predictions and experimental measurements for various W decay observables, the NNLO strong coupling constant at the Z pole, $\alpha_s(\rm m_Z) = 0.117 \pm 0.030_{\rm exp} \pm 0.003_{\rm th} \pm 0.001_{\rm par}$, as well as the charm-strange CKM element, $\rm V_{cs} = 0.973 \pm 0.003_{\rm exp} \pm 0.001_{\rm par}$, can be extracted under different assumptions. We also show that W decays provide today the most precise test of CKM unitarity for the 5 quarks lighter than $m_{\rm W}$, $\sum_{u,c,d,s,b} |V_{i,j}|^2 = 1.999 \pm 0.006_{\rm exp} \pm 0.001_{\rm th}$. Perspectives for $\alpha_s$ and $\rm V_{cs}$ extractions from W decays measurements at the LHC and future $e^+e^-$ colliders are presented. |
id | cern-2140736 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2016 |
record_format | invenio |
spelling | cern-21407362023-07-06T06:10:54Zdoi:10.1016/j.physletb.2016.10.012http://cds.cern.ch/record/2140736engd'Enterria, DavidSrebre, Matej$\alpha_s$ and |$\rm V_{cs}$| determination, and CKM unitarity test, from W decays at NNLOParticle Physics - PhenomenologyThe hadronic ($\Gamma^{\rm W}_{\rm had}$) and total ($\Gamma^{\rm W}_{\rm tot}$) widths of the W boson, computed at least at next-to-next-to-leading-order (NNLO) accuracy, are combined to derive a new precise prediction for the hadronic W branching ratio ${\cal B}^{\rm W}_{\rm had} \equiv \Gamma^{\rm W}_{\rm had}/\Gamma^{\rm W}_{\rm tot}$ = $0.682 \pm 0.011_{\rm par}$, using the experimental Cabibbo-Kobayashi-Maskawa (CKM) matrix elements, or ${\cal B}^{\rm W}_{\rm had} = 0.6742 \pm 0.0002_{\rm th} \pm 0.0001_{\rm par}$ assuming CKM unitarity, with uncertainties dominated by the input parameters of the calculations. Comparing the theoretical predictions and experimental measurements for various W decay observables, the NNLO strong coupling constant at the Z pole, $\alpha_s(\rm m_Z) = 0.117 \pm 0.030_{\rm exp} \pm 0.003_{\rm th} \pm 0.001_{\rm par}$, as well as the charm-strange CKM element, $\rm V_{cs} = 0.973 \pm 0.003_{\rm exp} \pm 0.001_{\rm par}$, can be extracted under different assumptions. We also show that W decays provide today the most precise test of CKM unitarity for the 5 quarks lighter than $m_{\rm W}$, $\sum_{u,c,d,s,b} |V_{i,j}|^2 = 1.999 \pm 0.006_{\rm exp} \pm 0.001_{\rm th}$. Perspectives for $\alpha_s$ and $\rm V_{cs}$ extractions from W decays measurements at the LHC and future $e^+e^-$ colliders are presented.The hadronic ( ΓhadW ) and total ( ΓtotW ) widths of the W boson, computed at least at next-to-next-to-leading-order (NNLO) accuracy, are combined to derive a new precise prediction for the hadronic W branching ratio BhadW ≡ ΓhadW/ΓtotW=0.682±0.011par , using the experimental Cabibbo–Kobayashi–Maskawa (CKM) matrix elements, with uncertainties dominated by the input parameters of the calculations, or BhadW=0.6742±0.0002th±0.0001par assuming CKM unitarity. Comparing the theoretical predictions and experimental measurements for various W decay observables, the NNLO strong coupling constant at the Z pole, αs(mZ2)=0.117±0.042exp±0.004th±0.001par , as well as the charm-strange CKM element, |Vcs|=0.973±0.004exp±0.002par , can be extracted under different assumptions. We also show that W decays provide today the most precise test of CKM unitarity for the 5 quarks lighter than mW , ∑u,c,d,s,b|Vij|2=1.999±0.008exp±0.001th . Perspectives for αs and |Vcs| extractions from W decays measurements at the LHC and future e+e− colliders are presented.The hadronic ($\Gamma^{\rm W}_{\rm had}$) and total ($\Gamma^{\rm W}_{\rm tot}$) widths of the W boson, computed at least at next-to-next-to-leading-order (NNLO) accuracy, are combined to derive a new precise prediction for the hadronic W branching ratio ${\cal B}^{\rm W}_{\rm had} \equiv \Gamma^{\rm W}_{\rm had}/\Gamma^{\rm W}_{\rm tot}$ = $0.682 \pm 0.011_{\rm par}$, using the experimental Cabibbo-Kobayashi-Maskawa (CKM) matrix elements, or ${\cal B}^{\rm W}_{\rm had} = 0.6742 \pm 0.0002_{\rm th} \pm 0.0001_{\rm par}$ assuming CKM unitarity, with uncertainties dominated by the input parameters of the calculations. Comparing the theoretical predictions and experimental measurements for various W decay observables, the NNLO strong coupling constant at the Z pole, $\alpha_s(m_Z) = 0.117 \pm 0.042_{\rm exp} \pm 0.004_{\rm th} \pm 0.001_{\rm par}$, as well as the charm-strange CKM element, $\rm V_{cs}$ = 0.973 $\pm$ 0.004$_{\rm exp}$ $\pm$ 0.002$_{\rm par}$, can be extracted under different assumptions. We also show that W decays provide today the most precise test of CKM unitarity for the 5 quarks lighter than $m_{\rm W}$, $\sum_{ u,c,d,s,b} |V_{ ij}|^2 = 1.999 \pm 0.008_{\rm exp} \pm 0.001_{\rm th}$. Perspectives for $\alpha_s$ and $\rm V_{cs}$ extractions from W decays measurements at the LHC and future $e^+e^-$ colliders are presented.arXiv:1603.06501oai:cds.cern.ch:21407362016-03-21 |
spellingShingle | Particle Physics - Phenomenology d'Enterria, David Srebre, Matej $\alpha_s$ and |$\rm V_{cs}$| determination, and CKM unitarity test, from W decays at NNLO |
title | $\alpha_s$ and |$\rm V_{cs}$| determination, and CKM unitarity test, from W decays at NNLO |
title_full | $\alpha_s$ and |$\rm V_{cs}$| determination, and CKM unitarity test, from W decays at NNLO |
title_fullStr | $\alpha_s$ and |$\rm V_{cs}$| determination, and CKM unitarity test, from W decays at NNLO |
title_full_unstemmed | $\alpha_s$ and |$\rm V_{cs}$| determination, and CKM unitarity test, from W decays at NNLO |
title_short | $\alpha_s$ and |$\rm V_{cs}$| determination, and CKM unitarity test, from W decays at NNLO |
title_sort | $\alpha_s$ and |$\rm v_{cs}$| determination, and ckm unitarity test, from w decays at nnlo |
topic | Particle Physics - Phenomenology |
url | https://dx.doi.org/10.1016/j.physletb.2016.10.012 http://cds.cern.ch/record/2140736 |
work_keys_str_mv | AT denterriadavid alphasandrmvcsdeterminationandckmunitaritytestfromwdecaysatnnlo AT srebrematej alphasandrmvcsdeterminationandckmunitaritytestfromwdecaysatnnlo |