Abstract

A study of the charged-particle density (number density) in the transverse region of the di-hadron correlations exploiting the existing pp and p$\bar{\rm p}$ data from RHIC to LHC energies is reported. This region has contributions from the Underlying Event (UE) as well as from Initial- and Final-State Radiation (ISR-FSR). Based on the data, a two-component model is built. This has the functional form $\propto s^{\alpha}+\beta\log(s)$, where the logarithmic (($\beta = 0.140 \pm 0.007$)) and the power-law ($\alpha = 0.270 \pm 0.005$) terms describe the components more sensitive to the ISR-FSR and UE contributions, respectively. The model describes the data from RHIC to LHC energies, the extrapolation to higher energies indicates that at around $\sqrt{s} \approx 100$\,TeV the number density associated to UE will match that from ISR-FSR. Although this behaviour is not predicted by PYTHIA~8.244, the power-law behaviour of the UE contribution is consistent with the energy dependence of the parameter that regulates Multiparton Interactions. Using simulations, KNO-like scaling properties of the multiplicity distributions in the regions sensitive to either UE or ISR-FSR are also discussed. The results presented here can be helpful to constrain QCD-inspired Monte Carlo models at the Future Circular Collider energies, as well as to characterize the UE-based event classifiers which are currently used at the LHC.

Highlights

  • The inelastic proton-proton cross section has contributions from diffractive and nondiffractive processes

  • Albeit in PYTHIA, the multiparton interactions (MPI)-sensitive region is well described by a power-law function (∝ s0.2p3)ffi,ffi such a contribution is found to increase faster with s in the datadriven model than in PYTHIA 8.244

  • It is worth mentioning that the exponent which was found for PYTHIA 8 is close to that which enters in the Monash tune for the parametrization of the energy dependence of MPI

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Summary

INTRODUCTION

The inelastic proton-proton (pp) cross section has contributions from diffractive (single-diffraction and doublediffraction) and nondiffractive processes. Inelastic pp collisions are selected using a minimum-bias trigger, while the UE has to be studied in events in which a hard scattering has occurred. This can be achieved by selecting events with a high transverse momentum (e.g., ptTrig ≥ 5 GeV=c) charged particle at midpseudorapidity. The available underlying-event data measured at the Relativistic Heavy Ion Collider (RHIC), the Tevatron, and the Large Hadron Collider (LHC) energies are investigated. The CDF Collaboration subdivided the transverse region into trans-max and trans-min in order to increase the sensitivity to ISR-FSR and UE (beam-beam remnant and MPI) effects, respectively [30].

UNDERLYING EVENT OBSERVABLES
RESULTS AND DISCUSSION
Filled area: data driven prediction
CONCLUSIONS
Full Text
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