TY - JOUR
T1 - High-precision measurement of the W boson mass with the CMS experiment
AU - The CMS collaboration
AU - Druzhkin, D.
AU - Borshch, V.
AU - Babaev, A.
AU - Uzunian, A.
AU - Slabospitskii, S.
AU - Kachanov, V.
AU - Skovpen, Y.
AU - Radchenko, O.
AU - Kozyrev, A.
AU - Dimova, T.
AU - Blinov, V.
AU - Vorotnikov, G.
AU - Volkov, P.
AU - Savrin, V.
AU - Perfilov, M.
AU - Lukina, O.
AU - Klyukhin, V.
AU - Dudko, L.
AU - Dubinin, M.
AU - Bunichev, V.
AU - Boos, E.
AU - Terkulov, A.
AU - Kirakosyan, M.
AU - Azarkin, M.
AU - Andreev, V.
AU - Polikarpov, S.
AU - Danilov, M.
AU - Chistov, R.
AU - Zhokin, A.
AU - Popov, V.
AU - Lychkovskaya, N.
AU - Gavrilov, V.
AU - Ivanov, K.
AU - Aushev, T.
AU - Toropin, A.
AU - Tlisova, I.
AU - Krasnikov, N.
AU - Kirsanov, M.
AU - Kirpichnikov, D.
AU - Karneyeu, A.
AU - Golubev, N.
AU - Gninenko, S.
AU - Dermenev, A.
AU - Andreev, Yu
AU - Vorobyev, A.
AU - Uvarov, L.
AU - Sulimov, V.
AU - Sosnov, D.
AU - Oreshkin, V.
AU - Bouhali, O.
N1 - Publisher Copyright:
© The Author(s) 2026.
PY - 2026/4/9
Y1 - 2026/4/9
N2 - In the standard model of particle physics, the masses of the W and Z bosons, the carriers of the weak interaction, are uniquely related. A precise determination of their masses is important because quantum loops of heavy, undiscovered particles could modify this relationship. Although the Z mass is known to the remarkable precision of 22 parts per million (2.0 MeV), the W mass is known much less precisely. A global fit to measured electroweak observables predicts the W mass with 6 MeV uncertainty1, 2–3. Reaching a comparable experimental precision would be a sensitive and fundamental test of the standard model, made even more urgent by a recent challenge to the global fit prediction by a measurement from the CDF Collaboration at the Fermilab Tevatron collider4. Here we report the measurement of the W mass by the CMS Collaboration at the CERN Large Hadron Collider, based on a large data sample of W → μν events collected in 2016 at the proton–proton collision energy of 13 TeV. The measurement exploits a high-granularity maximum likelihood fit to the kinematic properties of muons produced in W decays. By combining an accurate determination of experimental effects with marked in situ constraints of theoretical inputs, we reach a precise measurement of the W mass, of 80,360.2 ± 9.9 MeV, in agreement with the standard model prediction.
AB - In the standard model of particle physics, the masses of the W and Z bosons, the carriers of the weak interaction, are uniquely related. A precise determination of their masses is important because quantum loops of heavy, undiscovered particles could modify this relationship. Although the Z mass is known to the remarkable precision of 22 parts per million (2.0 MeV), the W mass is known much less precisely. A global fit to measured electroweak observables predicts the W mass with 6 MeV uncertainty1, 2–3. Reaching a comparable experimental precision would be a sensitive and fundamental test of the standard model, made even more urgent by a recent challenge to the global fit prediction by a measurement from the CDF Collaboration at the Fermilab Tevatron collider4. Here we report the measurement of the W mass by the CMS Collaboration at the CERN Large Hadron Collider, based on a large data sample of W → μν events collected in 2016 at the proton–proton collision energy of 13 TeV. The measurement exploits a high-granularity maximum likelihood fit to the kinematic properties of muons produced in W decays. By combining an accurate determination of experimental effects with marked in situ constraints of theoretical inputs, we reach a precise measurement of the W mass, of 80,360.2 ± 9.9 MeV, in agreement with the standard model prediction.
UR - https://www.scopus.com/pages/publications/105035376920
U2 - 10.1038/s41586-026-10168-5
DO - 10.1038/s41586-026-10168-5
M3 - Article
C2 - 41951965
AN - SCOPUS:105035376920
SN - 0028-0836
VL - 652
SP - 321
EP - 327
JO - Nature
JF - Nature
IS - 8109
ER -