• Open Access

B0B¯0 mixing: Matching to HQET at NNLO

Andrey G. Grozin, Thomas Mannel, and Alexei A. Pivovarov
Phys. Rev. D 98, 054020 – Published 24 September 2018

Abstract

We compute perturbative matching coefficients to the heavy quark effective theory (HQET) representation for the QCD effective local ΔB=2 Hamiltonian that determines the mass difference in the B0B¯0 system of states. We report on the results at next-to-next-to-leading order in the strong coupling constant for matching coefficients of two physical operators in HQET. Our results provide firm confirmation that the recent next-to-leading order sum rules analysis of the bag parameter Bq is stable with regard of inclusion of higher order radiative corrections. As a byproduct of our calculation we give a fully analytical solution for the one-loop QCD-to-HQET matching problem: we present the explicit formulas for the renormalization of four-quark operators of the full bases in both QCD and HQET and the expressions for matching coefficients in a closed form.

  • Received 19 June 2018

DOI:https://doi.org/10.1103/PhysRevD.98.054020

Published by the American Physical Society under the terms of the Creative Commons Attribution 4.0 International license. Further distribution of this work must maintain attribution to the author(s) and the published article’s title, journal citation, and DOI. Funded by SCOAP3.

Published by the American Physical Society

Physics Subject Headings (PhySH)

Particles & Fields

Authors & Affiliations

Andrey G. Grozin1,2,3,4, Thomas Mannel2, and Alexei A. Pivovarov2

  • 1PRISMA Cluster of Excellence, Johannes Gutenberg Universität, Staudingerweg 9, 55128 Mainz, Germany
  • 2Theoretische Elementarteilchenphysik, Naturwissenschaftlich-Technische Fakultät, Universität Siegen, Walter-Flex-Str. 3, 57068 Siegen, Germany
  • 3Budker Institute of Nuclear Physics SB RAS, Lavrentyev st. 11, Novosibirsk 630090, Russia
  • 4Novosibirsk State University, Pirogova st. 2, Novosibirsk 630090, Russia

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Issue

Vol. 98, Iss. 5 — 1 September 2018

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