Abstract

We report on the measurement of the Central Exclusive Production of charged particle pairs h+h− (h = π, K, p) with the STAR detector at RHIC in proton-proton collisions at sqrt{s} = 200 GeV. The charged particle pairs produced in the reaction pp → p′ + h+h− + p′ are reconstructed from the tracks in the central detector and identified using the specific energy loss and the time of flight method, while the forward-scattered protons are measured in the Roman Pot system. Exclusivity of the event is guaranteed by requiring the transverse momentum balance of all four final-state particles. Differential cross sections are measured as functions of observables related to the central hadronic final state and to the forward-scattered protons. They are measured in a fiducial region corresponding to the acceptance of the STAR detector and determined by the central particles’ transverse momenta and pseudorapidities as well as by the forward-scattered protons’ momenta. This fiducial region roughly corresponds to the square of the four-momentum transfers at the proton vertices in the range 0.04 GeV2< −t1, −t2< 0.2 GeV2, invariant masses of the charged particle pairs up to a few GeV and pseudorapidities of the centrally-produced hadrons in the range |η| < 0.7. The measured cross sections are compared to phenomenological predictions based on the Double Pomeron Exchange (DPE) model. Structures observed in the mass spectra of π+π− and K+K− pairs are consistent with the DPE model, while angular distributions of pions suggest a dominant spin-0 contribution to π+π− production. For π+π− production, the fiducial cross section is extrapolated to the Lorentz-invariant region, which allows decomposition of the invariant mass spectrum into continuum and resonant contributions. The extrapolated cross section is well described by the continuum production and at least three resonances, the f0(980), f2(1270) and f0(1500), with a possible small contribution from the f0(1370). Fits to the extrapolated differential cross section as a function of t1 and t2 enable extraction of the exponential slope parameters in several bins of the invariant mass of π+π− pairs. These parameters are sensitive to the size of the interaction region.

Highlights

  • Background estimationBackground in the analysis arises from non-exclusive processes leading to correlated signals in the Roman Pot (RP) and TOF/Time Projection Chamber (TPC) (‘single source’) and from coincidences of a signal in the RP with an uncorrelated signal in the TOF/TPC (‘pile-up’)

  • We report on the measurement of the Central Exclusive Production of charged particle pairs h+h− (h = π, K, p) with the STAR detector at RHIC in proton-proton

  • The forward-scattered protons are measured in the Roman Pot (RP) system adopted from the pp2pp experiment [44] at RHIC

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Summary

Introduction

Background estimationBackground in the analysis arises from non-exclusive processes leading to correlated signals in the RP and TOF/TPC (‘single source’) and from coincidences of a signal in the RP with an uncorrelated signal in the TOF/TPC (‘pile-up’). All the above sources of background are estimated using a data-driven method Both undetected particles in ‘single source’ events and the random character of ‘pile-up’ events lead to breaking the correlation between the central h+h− pair and the forward protons and to a much flatter pmTiss distribution. This can be seen in figure 5 (left column), where the pmTiss distribution starts to increase above 100 MeV. The shape of the background as a function of pmTiss is confirmed by MC predictions and like-sign events (shown by red points), which are, by definition, background. This background amounts to 5.3% (π+π−), 5.4% (K+K−) and 12% (pp)

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