High-order threshold corrections for top-pair and single-top production
DPF2015-76 May 11, 2018
High-order threshold corrections for top-pair
and single-top production
Department of Physics
Kennesaw State University, Kennesaw, GA 30144, USA
I present results for high-order corrections from threshold resummation to cross sections and differential distributions in top-antitop pair production and in single-top production. I show aNLO results for the total cross section as well as for the top-quark transverse-momentum () and rapidity distributions, and the top-quark forward-backward asymmetry in production. I compare with the most recent Tevatron and LHC data, including at 13 TeV. I also present aNNLO results for cross sections and distributions in -channel, -channel, and -channel single-top production.
The Meeting of the American Physical Society
Division of Particles and Fields
Ann Arbor, Michigan, August 4–8, 2015
Top-quark physics has been a centerpiece of high-energy collider experiments, first at the Tevatron and then at the LHC. The correct understanding of the production mechanisms of the top is thus of fundamental importance. Total cross sections and differential distributions of the top quark have been calculated to high theoretical precision and measured by the experiments.
In this talk I present the most recent and most accurate theoretical results for the production of top-antitop pairs, and for single top production. Soft-gluon threshold corrections are added at one order higher than known complete fixed-order results in each case. Thus, I present approximate NLO (aNLO) results for production  based on NNLL resummation . I show that they are in excellent agreement with recent LHC and Tevatron data [3, 4, 5, 6, 7, 8, 9, 10]. An expansion of the NNLL resummed cross section  is used through NLO in , thus avoiding the need for a prescription. We prefer fixed-order expansions  because the minimal or other prescriptions have chronically produced results that severely underestimate the size of the true cross section, while our fixed-order expansions have been exceedingly accurate in predicting the higher-order corrections. I also present approximate NNLO (aNNLO) results for single-top production  which are also in excellent agreement with recent LHC and Tevatron data [13, 14, 16, 15, 17].
2 Top-antitop pair production
I begin my presentation with aNLO results for production. MSTW2008 NNLO pdf  are used for all numerical results. I show in Fig. 1 the aNLO theoretical predictions for the total cross section as a function of LHC energy. The central result as well as the variations with scale and pdf uncertainties are shown. The theoretical predictions are compared with LHC data from ATLAS and CMS at 7 TeV  and 8 TeV , and with the newest data at 13 TeV  from Run 2 at the LHC. Remarkable agreement is found for all energies. The recent 13 TeV LHC data have of course still rather large uncertainties, much larger than those of theory. Also excellent agreement is found with 1.96 Tevatron data  as shown in .
Next I discuss the theoretical results for the distributions. In the left plot of Fig. 2, I show the central aNLO results for the top-quark transverse-momentum distributions at 7, 8, 13, and 14 TeV LHC energies. The right plot of Fig. 2 shows the normalized top-quark distributions at 8 TeV (bottom half) compared with CMS data in the dilepton (black) and lepton+jets (red) channels ; and at 13 TeV (top half) compared with CMS dilepton data . Excellent agreement is found between our aNLO results and the data at both energies (and also at 7 TeV as shown in ).
We continue with theoretical results for the rapidity distributions. In the left plot of Fig. 3, I show the central aNLO results for the top-quark rapidity distributions at 7, 8, 13, and 14 TeV LHC energies. The right plot of Fig. 3 shows the normalized top-quark rapidity distribution at 8 TeV (bottom half) compared with CMS data in the dilepton (black) and lepton+jets (red) channels ; and the normalized distribution of the absolute value of the top rapidity at 13 TeV (top half) compared with CMS dilepton data . Excellent agreement of aNLO theory with data is found at 8 TeV energy (as well as at 7 TeV ). At 13 TeV, the error bars of the data are large but there is good overall agreement with theory.
In Fig. 4, I present aNLO results for differential distributions at the Tevatron collider at 1.96 TeV energy. The left plot shows the top-quark distribution, with scale variation, which compares very well with data from D0  (the inset plot shows more clearly the high- region). The right plot of Fig. 4 shows the distribution of the absolute value of the top rapidity. Again, the comparison with D0 data  shows very good agreement.
The top-quark forward-backward asymmetry, , is defined by . Writing explicitly the perturbative series for numerator and denominator, including both electroweak and aNLO QCD corrections, we can write the expression for as
This expression can be further re-expanded and written as
|% Eq. (1)|
|% Eq. (2)|
3 Single-top production
Next, I discuss aNNLO results for single-top production at the LHC and the Tevatron.
In the left plot of Fig. 5, I display the aNNLO single-top total cross sections in the -channel, -channel, and -channel, as functions of collider energy. At 1.96 TeV Tevatron energy, I compare with -channel data from CDF and D0 . At 7 and 8 TeV LHC energies, I compare with -channel data from ATLAS and CMS  and with -channel data from ATLAS and CMS . At 8 TeV LHC energy I compare with -channel data from ATLAS and CMS . Finally, at 13 TeV LHC energy I compare with the very recent -channel data from CMS . Excellent agreement of theory with data is found for all collider energies.
In the right plot of Fig. 5 the aNNLO top-quark distributions in single-top production are displayed in all three channels. The -channel distribution is numerically the largest, followed by that for production, and last by the -channel distribution.
I have presented the latest theoretical results for top quark production, both in top-antitop pair and in single-top processes. For production, I have presented the total cross sections and the top quark differential distributions in and rapidity through aNLO at LHC and Tevatron energies, as well as the forward-backward asymmetry at the Tevatron. Results for single-top production have been presented through aNNLO for total cross sections and distributions. The high-order corrections are significant, and all theoretical results are in very good agreement with recent analyses from the LHC and the Tevatron.
- This material is based upon work supported by the National Science Foundation under Grant No. PHY 1519606.
- N. Kidonakis, Phys. Rev. D 90, 014006 (2014) [arXiv:1405.7046 [hep-ph]]; Phys. Rev. D 91, 031501(R) (2015) [arXiv:1411.2633 [hep-ph]]; Phys. Rev. D 91, 071502(R) (2015) [arXiv:1501.01581 [hep-ph]].
- N. Kidonakis, Phys. Rev. Lett. 102, 232003 (2009) [arXiv:0903.2561 [hep-ph]]; Phys. Rev. D 82, 114030 (2010) [arXiv:1009.4935 [hep-ph]]; Phys. Rev. D 84, 011504 (2011) [arXiv:1105.5167 [hep-ph]].
- ATLAS and CMS Collaborations, ATLAS-CONF-2012-134, CMS-PAS-TOP-12-003.
- ATLAS and CMS Collaborations, ATLAS-CONF-2014-054, CMS-PAS-TOP-14-016.
- ATLAS Collaboration, ATLAS-CONF-2015-033; CMS Collaboration, CMS-PAS-TOP-15-005.
- CDF and D0 collaborations, Phys. Rev. D 89, 072001 (2014) [arXiv:1309.7570[hep-ex]].
- CMS Collaboration, arXiv:1505.04480 [hep-ex].
- CMS Collaboration, CMS-PAS-TOP-15-010.
- D0 Collaboration, Phys. Rev. D 90, 092006 (2014) [arXiv:1401.5785 [hep-ex]].
- CDF Collaboration, Phys. Rev. D 87, 092002 (2013) [arXiv:1211.1003 [hep-ex]]; D0 Collaboration, Phys. Rev. D 90, 072011 (2014) [arXiv:1405.0421 [hep-ex]].
- N. Kidonakis, Phys. Rev. D 64, 014009 (2001) [hep-ph/0010002]; Phys. Rev. D 73, 034001 (2006) [hep-ph/0509079].
- N. Kidonakis, Phys. Rev. D 81, 054028 (2010) [arXiv:1001.5034 [hep-ph]]; Phys. Rev. D 82, 054018 (2010) [arXiv:1005.4451 [hep-ph]]; Phys. Rev. D 83, 091503 (2011) [arXiv:1103.2792 [hep-ph]]; Phys. Part. Nucl. 45, 714 (2014) [arXiv:1210.7813 [hep-ph]]; Phys. Rev. D 88, 031504 (2013) [arXiv:1306.3592 [hep-ph]].
- CDF and D0 Collaborations, arXiv:1503.05027 [hep-ex].
- ATLAS Collaboration, Phys. Rev. D 90, 112006 (2014) [arXiv:1406.7844 [hep-ex]]; CMS Collaboration, JHEP 12, 035 (2012) [arXiv:1209.4533 [hep-ex]]; ATLAS and CMS Collaborations, ATLAS-CONF-2013-098, CMS-PAS-TOP-12-002.
- ATLAS Collaboration, Phys. Lett. B 716, 142 (2012) [arXiv:1205.5764 [hep-ex]]; CMS Collaboration, Phys. Rev. Lett. 110, 022003 (2013) [arXiv:1209.3489 [hep-ex]]; ATLAS and CMS Collaborations, ATLAS-CONF-2014-052, CMS-PAS-TOP-14-009.
- ATLAS Collaboration, Phys. Lett. B 740, 118 (2015) [arXiv:1410.0647 [hep-ex]]; CMS Collaboration, CMS-PAS-TOP-13-009.
- CMS Collaboration, CMS-PAS-TOP-15-004.
- A.D. Martin, W.J. Stirling, R.S. Thorne, and G. Watt, Eur. Phys. J. C 63, 189 (2009) [arXiv:0901.0002 [hep-ph]].
- N. Kidonakis, PoS(DIS2015)169 [arXiv:1506.04068 [hep-ph]]; PoS(DIS2015)170 [arXiv:1506.04072 [hep-ph]]; PoS(RADCOR2015)033 [arXiv:1509.02528 [hep-ph]].