dc.contributor.author |
CMS Collaboration |
en_US |
dc.contributor.author |
Sirunyan, A. M. |
en_US |
dc.contributor.author |
DUBE, SOURABH |
en_US |
dc.contributor.author |
KANSAL, B. |
en_US |
dc.contributor.author |
KAPOOR, A. |
en_US |
dc.contributor.author |
KOTHEKAR, K. |
en_US |
dc.contributor.author |
PANDEY, S. |
en_US |
dc.contributor.author |
RANE, A. |
en_US |
dc.contributor.author |
RASTOGI, A. |
en_US |
dc.contributor.author |
SHARMA, SEEMA et al. |
en_US |
dc.date.accessioned |
2020-08-07T08:43:42Z |
|
dc.date.available |
2020-08-07T08:43:42Z |
|
dc.date.issued |
2020-07 |
en_US |
dc.identifier.citation |
Journal of High Energy Physics, 2020(7). |
en_US |
dc.identifier.issn |
1029-8479 |
en_US |
dc.identifier.issn |
1126-6708 |
en_US |
dc.identifier.uri |
http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/4942 |
|
dc.identifier.uri |
https://doi.org/10.1007/JHEP07(2020)125 |
en_US |
dc.description.abstract |
Measurements of the cross section for the production of top quark pairs in association with a pair of jets from bottom quarks (σtt¯bb¯¯¯) and in association with a pair of jets from quarks of any flavor or gluons (σtt¯jj) and their ratio are presented. The data were collected in proton-proton collisions at a center-of-mass energy of 13 TeV by the CMS experiment at the LHC in 2016 and correspond to an integrated luminosity of 35.9 fb−1. The measurements are performed in a fiducial phase space and extrapolated to the full phase space, separately for the dilepton and lepton+jets channels, where lepton corresponds to either an electron or a muon. The results of the measurements in the fiducial phase space for the dilepton and lepton+jets channels, respectively, are σtt¯jj = 2.36±0.02 (stat)±0.20 (syst) pb and 31.0±0.2 (stat)±2.9 (syst) pb, and for the cross section ratio 0.017 ± 0.001 (stat) ± 0.001 (syst) and 0.020 ± 0.001 (stat) ± 0.001 (syst). The values of σtt¯bb¯¯¯ are determined from the product of the σtt¯jj and the cross section ratio, obtaining, respectively, 0.040±0.002 (stat)±0.005 (syst) pb and 0.62±0.03 (stat)±0.07 (syst) pb. These measurements are the most precise to date and are consistent, within the uncertainties, with the standard model expectations obtained using a matrix element calculation at next-to-leading order in quantum chromodynamics matched to a parton shower. |
en_US |
dc.language.iso |
en |
en_US |
dc.publisher |
Springer Nature |
en_US |
dc.subject |
Hadron-Hadron scattering (experiments) |
en_US |
dc.subject |
Jets |
en_US |
dc.subject |
Top physics |
en_US |
dc.subject |
TOC-AUG-2020 |
en_US |
dc.subject |
2020 |
en_US |
dc.subject |
2020-AUG-WEEK1 |
en_US |
dc.title |
Measurement of the cross section for tt¯ production with additional jets and b jets in pp collisions at √s = 13 TeV |
en_US |
dc.type |
Article |
en_US |
dc.contributor.department |
Dept. of Physics |
en_US |
dc.identifier.sourcetitle |
Journal of High Energy Physics |
en_US |
dc.publication.originofpublisher |
Foreign |
en_US |