TY - JOUR
T1 - Measurement of the W-boson mass in pp collisions at root s=7 TeV with the ATLAS detector
AU - Aaboud, M.
AU - Aad, G.
AU - Abbott, B.
AU - Abdallah, J.
AU - Abdinov, O.
AU - Abeloos, B
AU - Abidi, S.H.
AU - Abouzeid, Ossama Sherif Alexander
AU - Abraham, NL
AU - Abramowicz, H.
AU - Abreu, H.
AU - Abreu, R.
AU - Abulaiti, Y.
AU - Acharya, B.S.
AU - Adachi, Shin-ichi
AU - Adamczyk, L.
AU - Adams, David L.
AU - Adelman, J.
AU - Adersberger, M.
AU - Adye, T.
AU - Affolder, A. A.
AU - Agatonovic-Jovin, T.
AU - Besjes, Geert-Jan
AU - Hansen, Peter Henrik
AU - Xella, Stefania
AU - Monk, James William
AU - Dam, Mogens
AU - Thiele, Fabian Alexander Jürgen
AU - Petersen, Troels Christian
AU - Hansen, Jørn Dines
AU - Stark, Simon Holm
AU - Galster, Gorm Aske Gram Krohn
AU - Alonso Diaz, Alejandro
AU - Wiglesworth, Graig
AU - de Almeida Dias, Flavia
AU - Hansen, Jørgen Beck
AU - Bajic, Milena
N1 - Erratum for 10.1140/epjc/s10052-018-6354-3
PY - 2018/2/1
Y1 - 2018/2/1
N2 - A measurement of the mass of the W boson is presented based on proton–proton collision data recorded in 2011 at a centre-of-mass energy of 7 TeV with the ATLAS detector at the LHC, and corresponding to 4.6fb-1 of integrated luminosity. The selected data sample consists of 7.8 × 10 6 candidates in the W→ μν channel and 5.9 × 10 6 candidates in the W→ eν channel. The W-boson mass is obtained from template fits to the reconstructed distributions of the charged lepton transverse momentum and of the W boson transverse mass in the electron and muon decay channels, yielding (Formula presented.) where the first uncertainty is statistical, the second corresponds to the experimental systematic uncertainty, and the third to the physics-modelling systematic uncertainty. A measurement of the mass difference between the W+ and W- bosons yields mW+-mW-=-29±28 MeV.
AB - A measurement of the mass of the W boson is presented based on proton–proton collision data recorded in 2011 at a centre-of-mass energy of 7 TeV with the ATLAS detector at the LHC, and corresponding to 4.6fb-1 of integrated luminosity. The selected data sample consists of 7.8 × 10 6 candidates in the W→ μν channel and 5.9 × 10 6 candidates in the W→ eν channel. The W-boson mass is obtained from template fits to the reconstructed distributions of the charged lepton transverse momentum and of the W boson transverse mass in the electron and muon decay channels, yielding (Formula presented.) where the first uncertainty is statistical, the second corresponds to the experimental systematic uncertainty, and the third to the physics-modelling systematic uncertainty. A measurement of the mass difference between the W+ and W- bosons yields mW+-mW-=-29±28 MeV.
U2 - 10.1140/epjc/s10052-017-5475-4
DO - 10.1140/epjc/s10052-017-5475-4
M3 - Journal article
C2 - 31265006
SN - 1434-6044
VL - 78
JO - The European Physical Journal C: Particles and Fields
JF - The European Physical Journal C: Particles and Fields
IS - 2
M1 - 110
ER -