Abstract

We perform for the first time a direct calculation of on-shell K → ππ hadronic matrix elements of chromomagnetic operators (CMO) in the Standard Model and beyond. To this end, we use the successful Dual QCD (DQCD) approach in which we also consider off-shell K − π matrix elements that allow the comparison with lattice QCD calculations presented recently by the ETM collaboration. Working in the SU(3) chiral limit, we find for the single B parameter BCMO = 0.33. Using the numerical results provided by the ETM collaboration we argue that only small corrections beyond that limit are to be expected. Our results are relevant for new physics scenarios in the context of the emerging ε′/ε anomaly strongly indicated within DQCD and supported by RBC-UKQCD lattice collaboration.

Highlights

  • Models the rescue comes from the modification of the Wilson coefficient of the dominant electroweak LR penguin operator Q8, and solutions through a modified contribution of the dominant QCD LR penguin operator Q6 could be considered [11]

  • We perform for the first time a direct calculation of on-shell K → ππ hadronic matrix elements of chromomagnetic operators (CMO) in the Standard Model and beyond

  • We use the successful Dual QCD (DQCD) approach in which we consider off-shell K − π matrix elements that allow the comparison with lattice QCD calculations presented recently by the ETM collaboration

Read more

Summary

Short-distance mixing pattern

The non-leading in N term should be dropped

Long-distance mixing pattern
Matching SD and LD patterns around one GeV
Chromomagnetic penguin operators in and beyond the Standard Model
Dual QCD
Chiral Quark Model
Lattice QCD
Summary and conclusion
Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.