Figure | Description |
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Pair production differential cross sections | |

Full phase-space normalised differential ttbar cross-section as a function of the transverse momentum of the top quark. The CMS and ATLAS results are compared to NNLO and approximate NNLO calculations. The values for the top-quark mass (mtop), the renormalisation (muR) and factorisation (muF) scales, and the choice of the PDF set used in each calculation are provided. The variable mT is defined as the square root of the sum of the squares of top-quark mass and the transverse momentum of the top quark. Both the CMS and ATLAS measurements are performed assuming a top-quark mass value of 172.5 GeV. The shaded bands show the total uncertainty on the data measurements in each bin. The lower panel shows the ratio of the data measurements and the approximate NNLO calculations to the full NNLO calculation. PNG November 2017 |

Full phase-space normalised differential ttbar cross-section as a function of the transverse momentum of the top quark. The CMS and ATLAS results are compared to NNLO and approximate NNLO calculations. The values for the top-quark mass (mtop), the renormalisation (muR) and factorisation (muF) scales, and the choice of the PDF set used in each calculation are provided. The variable mT is defined as the square root of the sum of the squares of top-quark mass and the transverse momentum of the top quark. Both the CMS and ATLAS measurements are performed assuming a top-quark mass value of 172.5 GeV. The shaded bands show the total uncertainty on the data measurements in each bin. The lower panel shows the ratio of the data measurements and the approximate NNLO calculations to the full NNLO calculation. PNG November 2016 |

Full phase-space normalised differential ttbar cross-section as a function of the transverse momentum of the top quark. The CMS and ATLAS results are compared to NNLO and approximate NNLO calculations. The shaded bands show the total uncertainty on the data measurements in each bin. The lower panel shows the ratio of the data measurements and the approximate NNLO calculations to the full NNLO calculation. The data are only shown up to 400 GeV, since the NNLO prediction is not available above this value. PNG November 2015 |

-- MartijnMulders - 2015-12-04

I | Attachment | History | Action | Size | Date | Who | Comment |
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ll_topH_pt_ll_rel_vscale_nov17.pdf | r1 | manage | 22.4 K | 2018-02-27 - 10:04 | MartijnMulders | ||

png | ll_topH_pt_ll_rel_vscale_nov17.png | r1 | manage | 388.8 K | 2018-02-27 - 10:04 | MartijnMulders | |

tt_xsec_diff_8TeV_toppt.pdf | r1 | manage | 22.0 K | 2015-12-04 - 20:09 | MartijnMulders | ||

png | tt_xsec_diff_8TeV_toppt.png | r1 | manage | 49.2 K | 2015-12-04 - 20:09 | MartijnMulders | |

tt_xsec_diff_8TeV_toppt_nov2016.pdf | r1 | manage | 22.4 K | 2017-01-23 - 17:33 | MartijnMulders | ||

png | tt_xsec_diff_8TeV_toppt_nov2016.png | r1 | manage | 50.7 K | 2017-01-23 - 17:33 | MartijnMulders |

This topic: LHCPhysics > LHCTopWG > LHCTopWGSummaryPlots > TtbarDifferential8TeVpTtopHistory

Topic revision: r3 - 2018-02-27 - MartijnMulders

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