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 1⁄2μbŠ, 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

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Summary

INTRODUCTION

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.

EXPERIMENTAL SETUP
DATA ANALYSIS
Track reconstruction
Muon pair selection
EXPECTED PAIR SOURCES
Physical μμ pair sources
Open Heavy flavor
Drell-Yan
Unphysical μμ pair sources
Hadron-hadron pairs
Muon-hadron pairs
Combinatorial pair background
SIMULATION FRAMEWORK
Correlated hadrons and combinatorial pair background
Normalizing hadron-hadron and muon-hadron pairs
Choice and normalization of the combinatorial pair background
Fit strategy
Fit function
Fit results
Signal extraction
10 Like-sign pairs in North muon arm acceptance
Bottom cross section
SYSTEMATIC UNCERTAINTIES
Shape of simulated distributions
Input hadron spectra
Hadron simulation
Charm and bottom simulation
ZYAM normalization
Hadron-hadron correlations from PYTHIA
Fitting
Normalization of cocktail components
Statistical uncertainty in fit result
Model dependence on bb
Model dependence on efficiency correction
Trigger efficiency
Reconstruction efficiency
Global normalization uncertainties
Azimuthal opening angle and pair distributions for μμ pairs from ccand pbTb
BOTTOM CROSS SECTION
PHENIX
Drell-Yan differential cross section
SUMMARY
Default PHENIX simulation framework
Findings
FastMC

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