The performance of missing transverse momentum reconstruction and its significance with the ATLAS detector using 140 fb of TeV collisions
ATLAS collaboration - arXiv preprint arXiv:2402.05858, 2024 - arxiv.org
This paper presents the reconstruction of missing transverse momentum ($ p_ {\text
{T}}^{\text {miss}} $) in proton-proton collisions, at a center-of-mass energy of 13 TeV. This is
a challenging task involving many detector inputs, combining fully calibrated electrons,
muons, photons, hadronically decaying $\tau $-leptons, hadronic jets, and soft activity from
remaining tracks. Possible double counting of momentum is avoided by applying a signal
ambiguity resolution procedure which rejects detector inputs that have already been used …
{T}}^{\text {miss}} $) in proton-proton collisions, at a center-of-mass energy of 13 TeV. This is
a challenging task involving many detector inputs, combining fully calibrated electrons,
muons, photons, hadronically decaying $\tau $-leptons, hadronic jets, and soft activity from
remaining tracks. Possible double counting of momentum is avoided by applying a signal
ambiguity resolution procedure which rejects detector inputs that have already been used …
[HTML][HTML] The performance of missing transverse momentum reconstruction and its significance with the ATLAS detector using 140 fb of TeV collisions
G Aad, E Aakvaag, BK Abbott, K Abeling, NJ Abicht… - 2024 - hal.science
This paper presents the reconstruction of missing transverse momentum ($ p_ {\text
{T}}^{\text {miss}} $) in proton-proton collisions, at a center-of-mass energy of 13 TeV. This is
a challenging task involving many detector inputs, combining fully calibrated electrons,
muons, photons, hadronically decaying $\tau $-leptons, hadronic jets, and soft activity from
remaining tracks. Possible double counting of momentum is avoided by applying a signal
ambiguity resolution procedure which rejects detector inputs that have already been used …
{T}}^{\text {miss}} $) in proton-proton collisions, at a center-of-mass energy of 13 TeV. This is
a challenging task involving many detector inputs, combining fully calibrated electrons,
muons, photons, hadronically decaying $\tau $-leptons, hadronic jets, and soft activity from
remaining tracks. Possible double counting of momentum is avoided by applying a signal
ambiguity resolution procedure which rejects detector inputs that have already been used …
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