| dc.contributor.author | Sirunyan, A. M | |
| dc.contributor.author | Tumasyan, A. | |
| dc.contributor.author | Adam, W. | |
| dc.contributor.author | Ambrogi, F. | |
| dc.contributor.author | Bergauer, T. | |
| dc.contributor.author | Dragicevic, M. | |
| dc.contributor.author | Erö, J. | |
| dc.contributor.author | Escalante Del Valle, A. | |
| dc.contributor.author | Flechl, M. | |
| dc.contributor.author | Frühwirth, R. | |
| dc.contributor.author | Jeitler, M. | |
| dc.contributor.author | Krammer, N. | |
| dc.contributor.author | Krätschmer, I. | |
| dc.contributor.author | Liko, D. | |
| dc.contributor.author | Madlener, T. | |
| dc.contributor.author | Mikulec, I. | |
| dc.contributor.author | Rad, N. | |
| dc.date.accessioned | 2021-09-20T17:28:46Z | |
| dc.date.available | 2021-09-20T17:28:46Z | |
| dc.date.issued | 2020-07-20 | |
| dc.identifier.uri | https://hdl.handle.net/1721.1/131578 | |
| dc.description.abstract | Abstract
Measurements of the cross section for the production of top quark pairs in association with a pair of jets from bottom quarks
σ
t
t
¯
b
b
¯
$$ \left({\sigma}_{\mathrm{t}\overline{\mathrm{t}}\mathrm{b}\overline{\mathrm{b}}}\right) $$
and in association with a pair of jets from quarks of any flavor or gluons
σ
t
t
¯
jj
$$ \left({\sigma}_{\mathrm{t}\overline{\mathrm{t}}\mathrm{jj}}\right) $$
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
σ
t
t
¯
jj
$$ {\sigma}_{\mathrm{t}\overline{\mathrm{t}}\mathrm{jj}} $$
= 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
σ
t
t
¯
b
b
¯
$$ {\sigma}_{\mathrm{t}\overline{\mathrm{t}}\mathrm{b}\overline{\mathrm{b}}} $$
are determined from the product of the
σ
t
t
¯
jj
$$ {\sigma}_{\mathrm{t}\overline{\mathrm{t}}\mathrm{jj}} $$
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.publisher | Springer Berlin Heidelberg | en_US |
| dc.relation.isversionof | https://doi.org/10.1007/JHEP07(2020)125 | en_US |
| dc.rights | Creative Commons Attribution | en_US |
| dc.rights.uri | https://creativecommons.org/licenses/by/4.0/ | en_US |
| dc.source | Springer Berlin Heidelberg | en_US |
| dc.title | Measurement of the cross section for tt¯$$ \mathrm{t}\overline{\mathrm{t}} $$ production with additional jets and b jets in pp collisions at s$$ \sqrt{s} $$ = 13 TeV | en_US |
| dc.type | Article | en_US |
| dc.identifier.citation | Journal of High Energy Physics. 2020 Jul 20;2020(7):125 | en_US |
| dc.contributor.department | Massachusetts Institute of Technology. Department of Physics | |
| dc.identifier.mitlicense | PUBLISHER_CC | |
| dc.eprint.version | Final published version | en_US |
| dc.type.uri | http://purl.org/eprint/type/JournalArticle | en_US |
| eprint.status | http://purl.org/eprint/status/PeerReviewed | en_US |
| dc.date.updated | 2020-07-25T04:00:24Z | |
| dc.language.rfc3066 | en | |
| dc.rights.holder | The Author(s) | |
| dspace.embargo.terms | N | |
| dspace.date.submission | 2020-07-25T04:00:24Z | |
| mit.license | PUBLISHER_CC | |
| mit.metadata.status | Authority Work and Publication Information Needed | |