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Measurement of the effective weak mixing angle in $p\bar{p}\rightarrow Z/γ^{*}\rightarrow e^{+}e^{-}$ events

D0 Collaboration

TL;DR

The paper reports a precision measurement of the effective weak mixing angle $\sin^2\theta_W^{\text{eff}}_{\ell}$ in $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV using $Z/\gamma^{*} \rightarrow e^+e^-$ events collected with the D0 detector, corresponding to $9.7\,\text{fb}^{-1}$ of data. The analysis exploits the forward-backward asymmetry $A_{FB}$ as a function of the dilepton invariant mass $M_{ee}$ around the $Z$ pole, with three event categories (CC-CC, CC-EC, EC-EC) and expanded electron acceptance; a new electron energy calibration reduces the dominant systematic from the energy scale. Detector modeling, data-driven background estimates, and MC corrections including NNLO QCD and PDF reweighting are combined to construct $A_{FB}$ templates for different input values of $\sin^2\theta_W^{\text{eff}}_{\ell}$ and extract the measurement via template fits. The result, $\sin^2\theta_W^{\text{eff}}_{\ell} = 0.23147 \pm 0.00047$, is the most precise determination from light-quark interactions to date and is consistent with the world average and LEP/SLD measurements.

Abstract

We present a measurement of the fundamental parameter of the standard model, the weak mixing angle, in $p\bar{p}\rightarrow Z/γ^{*}\rightarrow e^{+}e^{-}$ events at a center of mass energy of 1.96 TeV, using data corresponding to 9.7 fb$^{-1}$ of integrated luminosity collected by the D0 detector at the Fermilab Tevatron. The effective weak mixing angle is extracted from the forward-backward charge asymmetry as a function of the invariant mass around the Z boson pole. The measured value of $\sin^2θ_{\text{eff}}^{\text{$\ell$}}=0.23147 \pm 0.00047$ is the most precise measurement from light quark interactions to date, with a precision close to the best LEP and SLD results.

Measurement of the effective weak mixing angle in $p\bar{p}\rightarrow Z/γ^{*}\rightarrow e^{+}e^{-}$ events

TL;DR

The paper reports a precision measurement of the effective weak mixing angle in collisions at TeV using events collected with the D0 detector, corresponding to of data. The analysis exploits the forward-backward asymmetry as a function of the dilepton invariant mass around the pole, with three event categories (CC-CC, CC-EC, EC-EC) and expanded electron acceptance; a new electron energy calibration reduces the dominant systematic from the energy scale. Detector modeling, data-driven background estimates, and MC corrections including NNLO QCD and PDF reweighting are combined to construct templates for different input values of and extract the measurement via template fits. The result, , is the most precise determination from light-quark interactions to date and is consistent with the world average and LEP/SLD measurements.

Abstract

We present a measurement of the fundamental parameter of the standard model, the weak mixing angle, in events at a center of mass energy of 1.96 TeV, using data corresponding to 9.7 fb of integrated luminosity collected by the D0 detector at the Fermilab Tevatron. The effective weak mixing angle is extracted from the forward-backward charge asymmetry as a function of the invariant mass around the Z boson pole. The measured value of \ell is the most precise measurement from light quark interactions to date, with a precision close to the best LEP and SLD results.

Paper Structure

This paper contains 1 section, 4 equations, 2 figures, 1 table.

Table of Contents

  1. Acknowledgements

Figures (2)

  • Figure 1: (color online). Comparison between the $A_{FB}$ distributions measured in the background-subtracted data and the MC for the three kinematic regions, with the corresponding $\chi^2$ per degree of freedom. $\sin^2 \theta_{W}$ in the MC is 0.23139. The error bars are statistical only.
  • Figure 2: (color online). Comparison of measured $\sin^2\theta_{\text{eff}}^{\text{$\ell$}}$ with results from other experiments. The average is a combination of $A_{FB}^{0,\ell}$, $A_{l}(P_{\tau})$, $A_{lr}(\text{SLD})$, $A_{FB}^{0,b}$, $A_{FB}^{0,c}$, and $Q_{FB}^{\text{had}}$ measurements from the LEP and SLD Collaborations LEP-SLD.