6533b85efe1ef96bd12bff1c

RESEARCH PRODUCT

Two-parton contribution to the heavy-quark forward–backward asymmetry in NNLO QCD

Thomas GehrmannWerner BernreutherPierpaolo MastroliaPierpaolo MastroliaT. LeineweberEttore RemiddiR. HeineschRoberto Bonciani

subject

QuarkNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::Latticemedia_common.quotation_subjectNuclear TheoryFOS: Physical sciencesParton01 natural sciencesAsymmetrylaw.inventionNuclear physicsHigh Energy Physics - Phenomenology (hep-ph)law0103 physical sciencesPERTURBATIVE QCDNuclear Experiment010306 general physicsCollidermedia_commonCondensed Matter::Quantum GasesPhysicsQuantum chromodynamicsCouplingASYMMETRY IN NNLO QCD010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyResonanceObservableHigh Energy Physics - PhenomenologyHigh Energy Physics::ExperimentHEAVY QUARKSRADIATIVE CORRECTIONS

description

Forward-backward asymmetries, $A_{FB}^Q$, are important observables for the determination of the neutral-current couplings of heavy quarks in inclusive heavy quark production, $e^+ e^- \to \gamma^*, Z^* \to Q +X$. In view of the measurement perspectives on $A_{FB}^Q$ at a future linear collider, precise predictions of $A_{FB}^Q$ are required for massive quarks. We compute the contribution of the $Q \bar Q$ final state to $A_{FB}^Q$ to order $\as^2$ in the QCD coupling. We provide general formulae, and we show that this contribution to $A_{FB}^Q$ is infrared-finite. We evaluate these two-parton contributions for $b$ and $c$ quarks on and near the $Z$ resonance, and for $t$ quarks above threshold. Moreover, near the $t \bar t$ threshold we obtain, by expanding in the heavy-quark velocity $\beta$, an expression for $A_{FB}^{t \bar t}$ to order $\as^2$ and NNLL in $\beta$. This quantity is equal, to this order in $\beta$, to the complete forward-backward asymmetry $A_{FB}^t$.

https://doi.org/10.1016/j.nuclphysb.2006.05.031