Abstract
PHENIX reports differential cross sections of $\mu\mu$ pairs from semileptonic heavy-flavor decays and the Drell-Yan production mechanism measured in $p$$+$$p$ collisions at $\sqrt{s}=200$ GeV at forward and backward rapidity ($1.2<|\eta|<2.2$). The $\mu\mu$ pairs from $c\bar{c}$, $b\bar{b}$, and Drell-Yan are separated using a template fit to unlike- and like-sign muon pair spectra in mass and $p_T$. The azimuthal opening angle correlation between the muons from $c\bar{c}$ and $b\bar{b}$ decays and the pair-$p_T$ distributions are compared to distributions generated using {\sc pythia} and {\sc powheg} models, which both include next-to-leading order processes. The measured distributions for pairs from $c\bar{c}$ are consistent with {\sc pythia} calculations. The $c\bar{c}$ data presents narrower azimuthal correlations and softer $p_T$ distributions compared to distributions generated from {\sc powheg}. The $b\bar{b}$ data are well described by both models. The extrapolated total cross section for bottom production is $3.75{\pm}0.24({\rm stat}){\pm}^{0.35}_{0.50}({\rm syst}){\pm}0.45({\rm global})$[$\mu$b], which is consistent with previous measurements at the Relativistic Heavy Ion Collider in the same system at the same collision energy, and is approximately a factor of two higher than the central value calculated with theoretical models. The measured Drell-Yan cross section is in good agreement with next-to-leading-order quantum-chromodynamics calculations.
Highlights
Lepton pair spectra are a classic tool to study particle production in collisions of hadronic beams
The extrapolated total cross section for bottom production is 3.75 Æ 0.24ðstatÞ Æ00..3550 ðsystÞ Æ 0.45ðglobalÞ 1⁄2μb, which is consistent with previous measurements at the Relativistic Heavy Ion Collider in the same system at the same collision energy and is approximately a factor of 2 higher than the central value calculated with theoretical models
Mechanism in pþp Invariant yields of μμ pairs from ccand bbare measured as a function of Δφ and pT and compared to different models, PYTHIA and POWHEG
Summary
Lepton pair spectra are a classic tool to study particle production in collisions of hadronic beams. PHENIX adds a new measurement rapidity obtained in of the pþp μcμolpliasiironcsonattinpuuffisffim1⁄4a2t0f0orGweaVrd. PHENIX adds a new measurement rapidity obtained in of the pþp μcμolpliasiironcsonattinpuuffisffim1⁄4a2t0f0orGweaVrd With these data the contributions from ccand bbdecays and the Drell-Yan production mechanism can be separated and used to determine their differential cross sections as function of pair mass, pT and opening angle. ΜÆμÆ muon pairs from bottom decays arise from two separate mechanisms, (i) from a combination of B → μ and B → D → μ decay chains [36] or (ii) from decays following B0B0 oscillations [37] These two contributions dominate the high mass μÆμÆ spectrum, which allows a precise measurement of the bottom cross section.
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