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Study of double parton interactions in diphoton + dijet events in $p\bar{p}$ collisions at $\sqrt{s} = 1.96$ TeV

D0 Collaboration

TL;DR

This study measures double parton scattering in the gamma gamma + dijet final state using 8.7 fb^-1 of p-pbar data from the D0 detector at sqrt(s)=1.96 TeV. A data-driven technique compares DPS and DI events to extract the effective cross section sigma_eff, carefully accounting for acceptances, efficiencies, and photon purity to minimize theoretical uncertainties. The analysis yields sigma_eff = 19.3 ± 1.4 (stat) ± 7.8 (syst) mb and finds that about 21% of the selected events arise from DPS, consistent with prior DPS measurements across other final states and energies. The work demonstrates a robust, data-driven approach to characterizing DPS and informs understanding of parton spatial distribution in the nucleon.

Abstract

We use a sample of diphoton + dijet events to measure the effective cross section of double parton interactions, which is found to be $σ_{\rm eff} = 19.3$ $\pm$ $1.4({\rm stat})$ $\pm$ $7.8({\rm syst})$ mb. The sample was collected by the D0 detector at the Fermilab Tevatron collider in $p\bar{p}$ collisions at $\sqrt{s} = 1.96$ TeV and corresponds to an integrated luminosity of 8.7 fb$^{-1}$.

Study of double parton interactions in diphoton + dijet events in $p\bar{p}$ collisions at $\sqrt{s} = 1.96$ TeV

TL;DR

This study measures double parton scattering in the gamma gamma + dijet final state using 8.7 fb^-1 of p-pbar data from the D0 detector at sqrt(s)=1.96 TeV. A data-driven technique compares DPS and DI events to extract the effective cross section sigma_eff, carefully accounting for acceptances, efficiencies, and photon purity to minimize theoretical uncertainties. The analysis yields sigma_eff = 19.3 ± 1.4 (stat) ± 7.8 (syst) mb and finds that about 21% of the selected events arise from DPS, consistent with prior DPS measurements across other final states and energies. The work demonstrates a robust, data-driven approach to characterizing DPS and informs understanding of parton spatial distribution in the nucleon.

Abstract

We use a sample of diphoton + dijet events to measure the effective cross section of double parton interactions, which is found to be mb. The sample was collected by the D0 detector at the Fermilab Tevatron collider in collisions at TeV and corresponds to an integrated luminosity of 8.7 fb.

Paper Structure

This paper contains 19 sections, 15 equations, 5 figures, 8 tables.

Figures (5)

  • Figure 1: Schematic view of DP scattering processes producing $\gamma\gamma+{\rm dijet}$ final state. The $\gamma \gamma$ process is shown for the $q \bar{q}$ scattering (above, light, blue online) and box $gg$ diagram (below, light, blue online). The additional dijet scattering is a darker diagram (red online).
  • Figure 2: Fraction of the $gg \to \gamma\gamma$ contribution to the total direct cross section comprising the $q\bar{q} \to \gamma\gamma$ and $gg \to \gamma\gamma$ processes. $M_{\gamma \gamma}$ is the invariant mass of the diphoton.
  • Figure 4: A diagram illustrating the orientation of photon and jet transverse momenta vectors in $\gamma\gamma+{\rm dijet}$ events. Vectors $q_T^{~1}$ and $q_T^{~2}$ are the $p_T$ imbalance vectors of diphoton and dijet pairs, respectively.
  • Figure 5: The fit of the 1VTX data $\Delta S$ distribution with SP and DP templates to extract the DP fraction. The black points correspond to data, red boxes to the DP signal MIXDP model normalized to the $f_{\mathrm{DP}}$ fraction obtained from the fit, and the blue triangles are the SP background template (SP1VTX) normalized to its fraction ($1 -$$f_{\mathrm{DP}}$). The pink open boxes correspond to the sum of the signal and background (total).
  • Figure 6: Existing measurements of the effective cross section, $\sigma_{\rm eff}$, compared to the result presented here (AFS: no uncertainty is reported; UA2: only a lower limit is provided). Results of the measurements are grouped by the final state.