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On the threshold behaviour of heavy top production

Torbjörn Sjöstrand

Abstract

The observation of an excess of ttbar production in the threshold region, by CMS and ATLAS, has been interpreted as a toponium contribution, i.e. from below-threshold ttbar virtual states. The news here is the nontrivial experimental extraction of such a signal, not its existence as such. Indeed, already 35+ years ago an NRQCD Green's function approach was used to model the above- and below-threshold production of ttbar pairs in pp/ppbar collisions. The relevant cross section equations from that study are now (re-)implemented in the Pythia 8 event generator. While the above-threshold part is straightforward, the physical interpretation and modelling of below-threshold events is nontrivial, and a final prescription is cross-checked against two simpler ones. Cross sections and some event properties are presented.

On the threshold behaviour of heavy top production

Abstract

The observation of an excess of ttbar production in the threshold region, by CMS and ATLAS, has been interpreted as a toponium contribution, i.e. from below-threshold ttbar virtual states. The news here is the nontrivial experimental extraction of such a signal, not its existence as such. Indeed, already 35+ years ago an NRQCD Green's function approach was used to model the above- and below-threshold production of ttbar pairs in pp/ppbar collisions. The relevant cross section equations from that study are now (re-)implemented in the Pythia 8 event generator. While the above-threshold part is straightforward, the physical interpretation and modelling of below-threshold events is nontrivial, and a final prescription is cross-checked against two simpler ones. Cross sections and some event properties are presented.

Paper Structure

This paper contains 1 equation, 2 figures.

Figures (2)

  • Figure 1: The threshold behavior. (a) Analytical expressions for singlet and octet cases, $E = m_{{\mathrm t}\overline{\mathrm t}} - 2m_{{\mathrm t}}$. (b) Cross section in a four-mass scenario simulation for the expected singlet/octet mix, $E = \hat{m} - m_{{\mathrm t} 1} - m_{{\mathrm t} 2}$.
  • Figure 2: Example of event properties for the ${\mathrm t}\overline{\mathrm t}$ pair mass range $300 < \hat{m} < 400$ GeV. (a) Cross section $\mathrm{d}\sigma/\mathrm{d}\hat{m}$. (b) Cross section for the heavier and lighter of the ${\mathrm t}$ and $\overline{\mathrm t}$, respectively.