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Measurement of the top-quark pole mass in dileptonic tt¯+ 1-jet events at √s = 13 TeV with the ATLAS experiment ATLAS Collaboration
Abstract
A measurement of the top-quark pole mass m
pole
t
is presented in tt¯ events with an
additional jet, tt¯+ 1-jet, produced in pp collisions at √
s = 13 TeV. The data sample, recorded
with the ATLAS experiment during Run 2 of the LHC, corresponds to an integrated luminosity
of 140 fb−1
. Events with one electron and one muon of opposite electric charge in the final
state are selected to measure the tt¯+ 1-jet differential cross-section as a function of the inverse
of the invariant mass of the tt¯+ 1-jet system. Iterative Bayesian Unfolding is used to correct
the data to enable comparison with fixed-order calculations at next-to-leading-order accuracy
in the strong coupling. The process pp → ttj¯ (2 → 3), where top quarks are taken as stable
particles, and the process pp → b
¯bl+νl−νj¯ (2 → 7), which includes top-quark decays to the
dilepton final state and off-shell effects, are considered. The top-quark mass is extracted using
a χ
2 fit of the unfolded normalized differential cross-section distribution. The results obtained
with the 2 → 3 and 2 → 7 calculations are compatible within theoretical uncertainties,
providing an important consistency check. The more precise determination is obtained for the
2 → 3 measurement: m
pole
t = 170.7±0.3 (stat.)±1.4 (syst.)±0.3 (scale)±0.2 (PDF⊕αS) GeV,
which is in good agreement with other top-quark mass results.
Item Metadata
| Title |
Measurement of the top-quark pole mass in dileptonic tt¯+ 1-jet events at √s = 13 TeV with the ATLAS experiment
|
| Creator | |
| Publisher |
Springer Berlin Heidelberg
|
| Date Issued |
2025-12-03
|
| Description |
A measurement of the top-quark pole mass m
pole
t
is presented in tt¯ events with an
additional jet, tt¯+ 1-jet, produced in pp collisions at √
s = 13 TeV. The data sample, recorded
with the ATLAS experiment during Run 2 of the LHC, corresponds to an integrated luminosity
of 140 fb−1
. Events with one electron and one muon of opposite electric charge in the final
state are selected to measure the tt¯+ 1-jet differential cross-section as a function of the inverse
of the invariant mass of the tt¯+ 1-jet system. Iterative Bayesian Unfolding is used to correct
the data to enable comparison with fixed-order calculations at next-to-leading-order accuracy
in the strong coupling. The process pp → ttj¯ (2 → 3), where top quarks are taken as stable
particles, and the process pp → b
¯bl+νl−νj¯ (2 → 7), which includes top-quark decays to the
dilepton final state and off-shell effects, are considered. The top-quark mass is extracted using
a χ
2 fit of the unfolded normalized differential cross-section distribution. The results obtained
with the 2 → 3 and 2 → 7 calculations are compatible within theoretical uncertainties,
providing an important consistency check. The more precise determination is obtained for the
2 → 3 measurement: m
pole
t = 170.7±0.3 (stat.)±1.4 (syst.)±0.3 (scale)±0.2 (PDF⊕αS) GeV,
which is in good agreement with other top-quark mass results.
|
| Subject | |
| Genre | |
| Type | |
| Language |
eng
|
| Date Available |
2025-12-24
|
| Provider |
Vancouver : University of British Columbia Library
|
| Rights |
Attribution 4.0 International (CC BY 4.0)
|
| DOI |
10.14288/1.0451082
|
| URI | |
| Affiliation | |
| Citation |
Journal of High Energy Physics. 2025 Dec 03;2025(12):23
|
| Publisher DOI |
10.1007/JHEP12(2025)023
|
| Peer Review Status |
Reviewed
|
| Scholarly Level |
Faculty; Researcher
|
| Copyright Holder |
The Author(s)
|
| Rights URI | |
| Aggregated Source Repository |
DSpace
|
Item Media
Item Citations and Data
Rights
Attribution 4.0 International (CC BY 4.0)