Table of Contents
Fetching ...

Compatibility and combination of world W-boson mass measurements

Simone Amoroso, Nansi Andari, William Barter, Josh Bendavid, Maarten Boonekamp, Stephen Farry, Martin Gruenewald, Chris Hays, Ross Hunter, Jan Kretzschmar, Oliver Lupton, Martina Pili, Miguel Ramos Pernas, Boris Tuchming, Mika Vesterinen, Alessandro Vicini, Chen Wang, Menglin Xu

TL;DR

This work performs a global, PDF-aware combination of $m_W$ measurements from ATLAS, LHCb, CDF, and D0 (plus LEP) within a coherent model that propagates theory uncertainties and correlations. By emulating each experiment's measurement with a common production/decay description and accounting for detector- and PDF-related shifts, the authors quantify cross-experiment compatibility across multiple PDF sets, with CT18 generally most compatible due to its larger uncertainties. The full combination yields $m_W = 80394.6 \,\pm\, 11.5~\mathrm{MeV}$ under CT18 but with only $0.5\%$ compatibility, while removing the CDF result raises the compatibility to $91\%$ and gives $m_W = 80369.2 \pm 13.3~\mathrm{MeV}$, differing from the CDF value by $3.6\sigma$. The study highlights that PDF model dependence and correlation structure are crucial for precision world averages and that achieving a consistent, high-precision $m_W$ determination will require improved PDF treatments and cross-checks across experiments.

Abstract

The compatibility of W-boson mass measurements performed by the ATLAS, LHCb, CDF, and D0 experiments is studied using a coherent framework with theory uncertainty correlations. The measurements are combined using a number of recent sets of parton distribution functions (PDF), and are further combined with the average value of measurements from the Large Electron-Positron collider. The considered PDF sets generally have a low compatibility with a suite of global rapidity-sensitive Drell-Yan measurements. The most compatible set is CT18 due to its larger uncertainties. A combination of all mW measurements yields a value of mW = 80394.6 +- 11.5 MeV with the CT18 set, but has a probability of compatibility of 0.5% and is therefore disfavoured. Combinations are performed removing each measurement individually, and a 91% probability of compatibility is obtained when the CDF measurement is removed. The corresponding value of the W boson mass is 80369.2 +- 13.3 MeV, which differs by 3.6 sigma from the CDF value determined using the same PDF set.

Compatibility and combination of world W-boson mass measurements

TL;DR

This work performs a global, PDF-aware combination of measurements from ATLAS, LHCb, CDF, and D0 (plus LEP) within a coherent model that propagates theory uncertainties and correlations. By emulating each experiment's measurement with a common production/decay description and accounting for detector- and PDF-related shifts, the authors quantify cross-experiment compatibility across multiple PDF sets, with CT18 generally most compatible due to its larger uncertainties. The full combination yields under CT18 but with only compatibility, while removing the CDF result raises the compatibility to and gives , differing from the CDF value by . The study highlights that PDF model dependence and correlation structure are crucial for precision world averages and that achieving a consistent, high-precision determination will require improved PDF treatments and cross-checks across experiments.

Abstract

The compatibility of W-boson mass measurements performed by the ATLAS, LHCb, CDF, and D0 experiments is studied using a coherent framework with theory uncertainty correlations. The measurements are combined using a number of recent sets of parton distribution functions (PDF), and are further combined with the average value of measurements from the Large Electron-Positron collider. The considered PDF sets generally have a low compatibility with a suite of global rapidity-sensitive Drell-Yan measurements. The most compatible set is CT18 due to its larger uncertainties. A combination of all mW measurements yields a value of mW = 80394.6 +- 11.5 MeV with the CT18 set, but has a probability of compatibility of 0.5% and is therefore disfavoured. Combinations are performed removing each measurement individually, and a 91% probability of compatibility is obtained when the CDF measurement is removed. The corresponding value of the W boson mass is 80369.2 +- 13.3 MeV, which differs by 3.6 sigma from the CDF value determined using the same PDF set.
Paper Structure (23 sections, 10 equations, 10 figures, 28 tables)

This paper contains 23 sections, 10 equations, 10 figures, 28 tables.

Figures (10)

  • Figure 1: Comparisons between the CDF simulation Aaltonen:2013vwa and the LHC-TeV MWWG simulation for the $m_{\scriptsize\textrm{T}}$ (top) and $p_{\scriptsize\textrm{T}}^{\ell}$ (bottom) distributions.
  • Figure 2: Comparisons of the D0 PMCS and the LHC-TeV MWWG simulation for the $m_{\scriptsize\textrm{T}}$ (top) and $p_{\scriptsize\textrm{T}}^{\ell}$ (bottom) distributions.
  • Figure 3: Comparison of the published and MWWG simulated $p_{\scriptsize\textrm{T}}^{\ell}$ (top) and $m_{\scriptsize\textrm{T}}$ (bottom) distributions for ATLAS.
  • Figure 4: Distributions of generated $p_{\scriptsize\textrm{T}}^{W}$ for $W^\pm$ candidate events in $p\bar{p}$ collisions at CDF and D0 (top), and for $W^+$ and $W^-$ events at ATLAS (bottom). The distributions represent the best-fit model resulting from the analysis of $W$- and $Z$-boson data in the respective experiments, and are shown after all event selection requirements.
  • Figure 5: PDF uncertainty correlation matrices for the CT18, MSHT20, NNPDF4.0, and ABMP16 PDF sets, in order from top to bottom.
  • ...and 5 more figures