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Heavy quarkonium in the saturated environment of high-multiplicity pp collisions
Journal
Physical Review D
Date Issued
2020-03-01
Author(s)
Pirner, H. J.
Potashnikova, I. K.
Reygers, K.
Abstract
High-multiplicity pp collisions exhibit features, traditionally associated with nuclear effects. Coherence
motivates to treat high-multiplicity pp, pA, and AA collisions on an equal footing. We rely on the
phenomenological parametrization for mean multiplicities of light hadrons and J=ψ, assuming their linear
dependence on Ncoll in pA collisions. The results of this approach underestimate the recently measured
production rate of J=ψ at very high hadronic multiplicities. The linear dependence of J=ψ multiplicity on
Ncoll is subject to predicted nonlinear corrections, related to mutual boosting of the saturation scales in
colliding dense parton clouds. A parameter-free calculation of the nonlinear corrections allows us to
explain data for pT-integrated yield of J=ψ at high hadronic multiplicities. Calculations are in a good
accord with data binned in several pT intervals as well. As was predicted, ϒ and J=ψ are equally suppressed
at forward rapidities in pA collisions. Consequently, their fractional multiplicities at forward rapidities in
pp collisions are equal as well, and their magnitude agrees with data.
motivates to treat high-multiplicity pp, pA, and AA collisions on an equal footing. We rely on the
phenomenological parametrization for mean multiplicities of light hadrons and J=ψ, assuming their linear
dependence on Ncoll in pA collisions. The results of this approach underestimate the recently measured
production rate of J=ψ at very high hadronic multiplicities. The linear dependence of J=ψ multiplicity on
Ncoll is subject to predicted nonlinear corrections, related to mutual boosting of the saturation scales in
colliding dense parton clouds. A parameter-free calculation of the nonlinear corrections allows us to
explain data for pT-integrated yield of J=ψ at high hadronic multiplicities. Calculations are in a good
accord with data binned in several pT intervals as well. As was predicted, ϒ and J=ψ are equally suppressed
at forward rapidities in pA collisions. Consequently, their fractional multiplicities at forward rapidities in
pp collisions are equal as well, and their magnitude agrees with data.
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