Abstract
Exclusive dimuon production in ultraperipheral collisions (UPC), resulting from photon-photon interactions in the strong electromagnetic fields of colliding high-energy lead nuclei, $\mathrm{PbPb}(\gamma\gamma) \rightarrow \mu^+\mu^- (\mathrm{Pb}^{(\star)}\mathrm{Pb}^{(\star)} )$, is studied using $\mathcal{L}_{\mathrm{int}} = 0.48$ nb$^{-1}$ of $\sqrt{s_\mathrm{NN}}=5.02$ TeV lead-lead collision data at the LHC with the ATLAS detector. Dimuon pairs are measured in the fiducial region $p_{\mathrm{T}\mu} > 4$ GeV, $|\eta_{\mu}| < 2.4$, invariant mass $m_{\mu\mu} > 10$ GeV, and $p_{\mathrm{T,\mu\mu}} < 2$ GeV. The primary background from single-dissociative processes is extracted from the data using a template fitting technique. Differential cross sections are presented as a function of $m_{\mu\mu}$, absolute pair rapidity ($|y_{\mu\mu}|$), scattering angle in the dimuon rest frame ($|\cos \vartheta^{\star}_{\mu\mu}|$) and the colliding photon energies. The total cross section of the UPC $\gamma \gamma \rightarrow \mu^{+}\mu^{-}$ process in the fiducial volume is measured to be $\sigma_{\mathrm{fid}}^{\mu\mu} = 34.1 \! \pm \! 0.3 \mathrm{(stat.)} \! \pm \! 0.7 \mathrm{(syst.)}$ $\mu\mathrm{b}$. Generally good agreement is found with calculations from STARlight, which incorporate the leading-order Breit-Wheeler process with no final-state effects, albeit differences between the measurements and theoretical expectations are observed. In particular, the measured cross sections at larger $|y_{\mu\mu}|$ are found to be about 10-20% larger in data than in the calculations, suggesting the presence of larger fluxes of photons in the initial state. Modification of the dimuon cross sections in the presence of forward and/or backward neutron production is also studied and is found to be associated with a harder incoming photon spectrum, consistent with expectations.
Highlights
Collisions of nuclei at ultrarelativistic energies are typically studied for processes in which the nucleons interact hadronically at impact parameters less than twice the nuclear radius (b < 2RA), producing a large volume of hot, dense quark-gluon plasma in the overlap region, which can decay into thousands of outgoing hadrons
This paper presents measurements of cross sections for exclusive dimuon production in ultraperipheral” collisions (UPC) with lead nuclei, PbPb(γ γ ) → μ+μ−(Pb( )Pb( )), using Lint = 0.48 nb−1 of data taken in 2015
We present comparisons of data with STARlight 2.0, which implements all of the primary physics mechanisms, except dissociative processes and QED final-state radiation (FSR)
Summary
Collisions of nuclei at ultrarelativistic energies are typically studied for processes in which the nucleons interact hadronically at impact parameters less than twice the nuclear radius (b < 2RA), producing a large volume of hot, dense quark-gluon plasma in the overlap region, which can decay into thousands of outgoing hadrons. The two muon four-momenta can be combined to present cross sections as a function of the maximum and minimum energies of the incoming photons Detailed comparisons of these data with predictions from STARlight provide the first detailed comparison at LHC energies of the various aspects of STARlight—from the nuclear photon fluxes to the implementation of the exclusivity condition—with experimental data over a very wide range in initial photon energies (up to 100 GeV). Cross sections for events with no forward neutron activity, which removes dissociative events, are presented as a function of dimuon acoplanarity These data can be used to study the impact of QED showering on the final-state muons in a environment with very low backgrounds.
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