Two-Parton Contribution to the Heavy-Quark Forward-Backward Asymmetry in NNLO QCD
| dc.creator | Bernreuther, W. | |
| dc.creator | Bonciani, R. | |
| dc.creator | Gehrmann, T. | |
| dc.creator | Leineweber, R. Heinesch T. | |
| dc.creator | Mastrolia, P. | |
| dc.creator | Remiddi, E. | |
| dc.date | 2006-04-04 | |
| dc.date.accessioned | 2026-07-07T10:44:58Z | |
| dc.date.available | 2026-07-07T10:44:58Z | |
| dc.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, $e^+ e^- \to γ^*, Z^* \to Q +X$. 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 $β$, an expression for $A_{FB}^{t \bar t}$ to order $\as^2$ and NNLL in $β$. This quantity is equal, to this order in $β$, to the complete forward-backward asymmetry $A_{FB}^t$. | |
| dc.description | latex, 26 pages, 2 tables, 17 figures | |
| dc.identifier | https://arxiv.org/abs/hep-ph/0604031 | |
| dc.identifier | http://arxiv.org/abs/hep-ph/0604031 | |
| dc.identifier | Nucl.Phys.B750:83-107,2006 | |
| dc.identifier | doi:10.1016/j.nuclphysb.2006.05.031 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/182781 | |
| dc.subject | High Energy Physics - Phenomenology | |
| dc.title | Two-Parton Contribution to the Heavy-Quark Forward-Backward Asymmetry in NNLO QCD | |
| dc.type | text |