Cargando…
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...
Autores principales: | , |
---|---|
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 |
_version_ | 1780886089640181760 |
---|---|
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 ($\approx -20\%$). |
id | cern-259672 |
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 |