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QCD corrections to inclusive $\Delta$S = 1,2 transitions at the next-to-leading order

The 2--point functions for $\Delta S=1$ current-current and QCD-penguin operators, as well as for the $\ds$ operator, are calculated at the next-to-leading order. The calculation is performed in two different renormalization schemes for $\gamma_5$, and the compatibility of the results obtained in th...

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Detalles Bibliográficos
Autores principales: Jamin, Matthias, Pich, Antonio
Lenguaje:eng
Publicado: 1994
Materias:
Acceso en línea:https://dx.doi.org/10.1016/0550-3213(94)90171-6
http://cds.cern.ch/record/259672
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author Jamin, Matthias
Pich, Antonio
author_facet Jamin, Matthias
Pich, Antonio
author_sort Jamin, Matthias
collection CERN
description The 2--point functions for $\Delta S=1$ current-current and QCD-penguin operators, as well as for the $\ds$ operator, are calculated at the next-to-leading order. The calculation is performed in two different renormalization schemes for $\gamma_5$, and the compatibility of the results obtained in the two schemes is verified. The scale- and scheme-invariant combinations of spectral 2--point functions and corresponding Wilson-coefficients are constructed and analyzed. For $\Delta S=1$, the QCD corrections to the CP-conserving part, dominated by current-current operators, are 40\%--120\% at $q^2=\left(1-3\,\mbox{\rm GeV}\right)^2$, whereas the correction to the imaginary part, mainly coming from the penguin operator $Q_6$, are 100\%--240\%. The large size of the gluonic corrections to current-current operators provides a qualitative understanding of the observed enhancement of $\Delta I=1/2$ transitions. In the $\Delta S=2$ sector the QCD corrections are quite moderate ($\approx -20\%$).
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1994
record_format invenio
spelling cern-2596722023-03-14T19:27:29Zdoi:10.1016/0550-3213(94)90171-6http://cds.cern.ch/record/259672engJamin, MatthiasPich, AntonioQCD corrections to inclusive $\Delta$S = 1,2 transitions at the next-to-leading orderParticle Physics - TheoryThe 2--point functions for $\Delta S=1$ current-current and QCD-penguin operators, as well as for the $\ds$ operator, are calculated at the next-to-leading order. The calculation is performed in two different renormalization schemes for $\gamma_5$, and the compatibility of the results obtained in the two schemes is verified. The scale- and scheme-invariant combinations of spectral 2--point functions and corresponding Wilson-coefficients are constructed and analyzed. For $\Delta S=1$, the QCD corrections to the CP-conserving part, dominated by current-current operators, are 40\%--120\% at $q^2=\left(1-3\,\mbox{\rm GeV}\right)^2$, whereas the correction to the imaginary part, mainly coming from the penguin operator $Q_6$, are 100\%--240\%. The large size of the gluonic corrections to current-current operators provides a qualitative understanding of the observed enhancement of $\Delta I=1/2$ transitions. In the $\Delta S=2$ sector the QCD corrections are quite moderate ($\approx -20\%$).The 2--point functions for $\Delta S=1$ current-current and QCD-penguin operators, as well as for the $\ds$ operator, are calculated at the next-to-leading order. The calculation is performed in two different renormalization schemes for $\gamma_5$, and the compatibility of the results obtained in the two schemes is verified. The scale- and scheme-invariant combinations of spectral 2--point functions and corresponding Wilson-coefficients are constructed and analyzed. For $\Delta S=1$, the QCD corrections to the CP-conserving part, dominated by current-current operators, are 40\%--120\% at $q~2=\left(1-3\,\mbox{\rm GeV}\right)~2$, whereas the correction to the imaginary part, mainly coming from the penguin operator $Q_6$, are 100\%--240\%. The large size of the gluonic corrections to current-current operators provides a qualitative understanding of the observed enhancement of $\Delta I=1/2$ transitions. In the $\Delta S=2$ sector the QCD corrections are quite moderate ($\approx -20\%$).The two-point functions for ΔS = 1 current-current and QCD-penguin operators, as well as for the ΔS = 2 operator, are calculated at the next-to-leading order. The calculation is performed in two different renormalization schemes for γ 5 , and the compatibility of the results obtained in the two schemes is verified. The scale- and scheme-invariant combinations of spectral two-point functions and corresponding Wilson coefficients are constructed and analyzed. For ΔS = 1, the QCD corrections to the CP -conserving part, dominated by current-current operators, are 40–120% at q 2 = (1–3 GeV) 2 , whereas the corrections to the imaginary part, mainly coming from the penguin operator Q 6 , are 100–240%. The large size of the gluonic corrections to current-current operators provides a qualitative understanding of the observed enhancement of ΔI = 1 2 transitions. In the ΔS = 2 sector the QCD corrections are quite moderate (≈−20%).hep-ph/9402363CERN-TH-7151-94FTUV-94-06IFIC-94-03CERN-TH-7151-94FTUV-94-6IFIC-94-3oai:cds.cern.ch:2596721994
spellingShingle Particle Physics - Theory
Jamin, Matthias
Pich, Antonio
QCD corrections to inclusive $\Delta$S = 1,2 transitions at the next-to-leading order
title QCD corrections to inclusive $\Delta$S = 1,2 transitions at the next-to-leading order
title_full QCD corrections to inclusive $\Delta$S = 1,2 transitions at the next-to-leading order
title_fullStr QCD corrections to inclusive $\Delta$S = 1,2 transitions at the next-to-leading order
title_full_unstemmed QCD corrections to inclusive $\Delta$S = 1,2 transitions at the next-to-leading order
title_short QCD corrections to inclusive $\Delta$S = 1,2 transitions at the next-to-leading order
title_sort qcd corrections to inclusive $\delta$s = 1,2 transitions at the next-to-leading order
topic Particle Physics - Theory
url https://dx.doi.org/10.1016/0550-3213(94)90171-6
http://cds.cern.ch/record/259672
work_keys_str_mv AT jaminmatthias qcdcorrectionstoinclusivedeltas12transitionsatthenexttoleadingorder
AT pichantonio qcdcorrectionstoinclusivedeltas12transitionsatthenexttoleadingorder