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The forward-backward asymmetry at NNLO revisited

Stefan Weinzierl

TL;DR

This work revisits the forward-backward asymmetry for flavoured quarks in e+e- annihilation and introduces an infrared-safe observable defined via flavoured quark jets using the flavour-k_perp algorithm. It computes the NLO and NNLO QCD corrections within a subtraction framework, leveraging a general NNLO program for e+e- → 2 jets, and carefully treats four-quark final states. The results show small NNLO corrections, especially under stringent two-jet cuts, indicating the observable can support high-precision measurements at future linear colliders. By resolving IR-safety issues, the approach provides a robust path to precise determinations of electroweak parameters from heavy-quark asymmetries.

Abstract

I reconsider the forward-backward asymmetry for flavoured quarks in electron-positron annihilation. I suggest an infrared-safe definition of this observable, such that the asymmetry may be computed in perturbative QCD with massless quarks. With this definition, the first and second order QCD corrections are computed.

The forward-backward asymmetry at NNLO revisited

TL;DR

This work revisits the forward-backward asymmetry for flavoured quarks in e+e- annihilation and introduces an infrared-safe observable defined via flavoured quark jets using the flavour-k_perp algorithm. It computes the NLO and NNLO QCD corrections within a subtraction framework, leveraging a general NNLO program for e+e- → 2 jets, and carefully treats four-quark final states. The results show small NNLO corrections, especially under stringent two-jet cuts, indicating the observable can support high-precision measurements at future linear colliders. By resolving IR-safety issues, the approach provides a robust path to precise determinations of electroweak parameters from heavy-quark asymmetries.

Abstract

I reconsider the forward-backward asymmetry for flavoured quarks in electron-positron annihilation. I suggest an infrared-safe definition of this observable, such that the asymmetry may be computed in perturbative QCD with massless quarks. With this definition, the first and second order QCD corrections are computed.

Paper Structure

This paper contains 5 sections, 22 equations, 4 tables.