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First Measurement of the Angular Coefficients of Drell-Yan $e^{+}e^{-}$ pairs in the Z Mass Region from $p\bar{p}$ Collisions at $\sqrt{s}$ = 1.96 TeV

CDF Collaboration, T. Aaltonen

TL;DR

The angular distributions are studied as a function of the transverse momentum of the electron-positron pair and show good agreement with the Lam-Tung relation, consistent with a spin-1 description of the gluon.

Abstract

We report on the first measurement of the angular distributions of final state electrons in $p\bar{p}\to γ^{*}/Z\to e^{+}e^{-}+X$ events produced in the $Z$ boson mass region at $\sqrt{s}=1.96$ TeV. The data sample collected by the CDF II detector for this result corresponds to 2.1 fb$^{-1}$ of integrated luminosity. The angular distributions are studied as a function of the transverse momentum of the electron-positron pair and show good agreement with the Lam-Tung relation, consistent with a spin-1 description of the gluon, and demonstrate that at high values of the transverse momentum, $Z$ bosons are produced via quark anti-quark annihilation and quark-gluon Compton processes.

First Measurement of the Angular Coefficients of Drell-Yan $e^{+}e^{-}$ pairs in the Z Mass Region from $p\bar{p}$ Collisions at $\sqrt{s}$ = 1.96 TeV

TL;DR

The angular distributions are studied as a function of the transverse momentum of the electron-positron pair and show good agreement with the Lam-Tung relation, consistent with a spin-1 description of the gluon.

Abstract

We report on the first measurement of the angular distributions of final state electrons in events produced in the boson mass region at TeV. The data sample collected by the CDF II detector for this result corresponds to 2.1 fb of integrated luminosity. The angular distributions are studied as a function of the transverse momentum of the electron-positron pair and show good agreement with the Lam-Tung relation, consistent with a spin-1 description of the gluon, and demonstrate that at high values of the transverse momentum, bosons are produced via quark anti-quark annihilation and quark-gluon Compton processes.

Paper Structure

This paper contains 1 equation, 3 figures, 1 table.

Figures (3)

  • Figure 1: Di-electron $P_{T}$ spectrum of data, default (CDF Tuned) pythia prediction, and backgrounds (QCD and electroweak process). The mass range corresponds to $66 < M_{ee} < 116$ GeV/c$^{2}$.
  • Figure 2: The $\cos\theta$ distribution of data and default (CDF Tuned) pythia prediction.
  • Figure 3: Comparison of the measured values of $A_0$, $A_2$, $A_3$ and $A_4$ (for $66<M_{ee}<116$ GeV/c$^2$), shown with statistical and systematic uncertainties combined in quadrature, to theory predictions. The data are plotted at the mean $P_T$ of the events for each bin. The last bin corresponds to $P_T > 55$ GeV/c with no upper limit. The horizontal uncertainty is RMS of the transverse momenta in each bin. Agreement chi is found with the predictions of fewz and powheg (shown) , and also with dyrad , madgraph , and pythia $~Z$ +1-jet MC (not shown). The data do not favor chi the predictions of default pythia , and vbp . Also shown are the pure $q\bar{q}\to \gamma^{*}/Z~G$ annihilation diagram prediction and the $qG \to \gamma^{*}/Z~q$ Compton process prediction from the pythia $~Z$ +1-jet MC.