Abstract
The production of χ_{c1}(3872) and ψ(2S) hadrons is studied as a function of charged particle multiplicity in pp collisions at a center-of-mass energy of 8TeV, corresponding to an integrated luminosity of 2 fb^{-1}. For both states, the fraction that is produced promptly at the collision vertex is found to decrease as charged particle multiplicity increases. The ratio of χ_{c1}(3872) to ψ(2S) cross sections for promptly produced particles is also found to decrease with multiplicity, while no significant dependence on multiplicity is observed for the equivalent ratio of particles produced away from the collision vertex in b-hadron decays. This behavior is consistent with a calculation that models the χ_{c1}(3872) structure as a compact tetraquark. Comparisons with model calculations and implications for the binding energy of the χ_{c1}(3872) state are discussed.
Highlights
In recent years, multiple new resonances containing heavy quarks have been observed that do not fit into the framework of conventional hadrons, see Ref. [1] for a recent review
LHCb has since measured the quantum numbers to be JPC 1⁄4 1þþ [8], which disfavors its assignment as conventional charmonium because no compatible charmonium states with these quantum numbers are expected near the measured mass [9]
As the effects governing heavy quark production and transport through the nucleus are assumed to be similar for states with the same quark content, the mechanism for the suppression of excited states is expected to occur in the late stages of the collision, after the heavy quark pair has hadronized into a final state
Summary
Multiple new resonances containing heavy quarks have been observed that do not fit into the framework of conventional hadrons, see Ref. [1] for a recent review. Ψð2SÞ states, fprompt, that are produced promptly at the pp collision vertex as a function of charged particle multiplicity are presented.
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