Measurement of jet photoproduction in ultra-peripheral Pb+Pb collisions without nuclear breakup at $\sqrt{s_{\mathrm{N}\mathrm{N}}}=5.02$ TeV with the ATLAS detector

In ultra-relativistic heavy ion collisions at the LHC, each nucleus acts as a source of high-energy quasi-real photons that can participate in scattering processes without causing either participating nucleus to break up and emit forward neutrons. This paper extends recent measurements of $\gamma +A\to \mathrm{j}\mathrm{e}\mathrm{t}\mathrm{s}$ production in ultra-peripheral Pb+Pb collisions at $\sqrt{s_{\mathrm{N}\mathrm{N}}}=5.02$ TeV with forward neutron emission on exactly one side of the event. The data presented here was recorded by the ATLAS collaboration at the LHC in 2018, corresponding to a luminosity of $1.72$ nb${}^{-1}$. These results examines $5.02$ TeV Pb+Pb collisions where neither nucleus breaks up ($0n0n$), providing a mixture of photon–pomeron ($\gamma +I\text{\hspace{0.17em}⁣}\text{\hspace{0.17em}⁣}P\to \mathrm{j}\mathrm{e}\mathrm{t}\mathrm{s}$), photon–photon ($\gamma +\gamma \to \mathrm{j}\mathrm{e}\mathrm{t}\mathrm{s}$), and peripheral photonuclear ($\gamma +A\to \mathrm{j}\mathrm{e}\mathrm{t}\mathrm{s}$) events. The different processes are statistically separated via a template fit of the minimum rapidity gap distribution. The kinematics of the hard processes are determined from $R=0.4$ jets reconstructed using the anti-$k_t$ algorithm. The statistical separation of the different processes then allows for the first measurement of $\gamma +I\text{\hspace{0.17em}⁣}\text{\hspace{0.17em}⁣}P\to \mathrm{j}\mathrm{e}\mathrm{t}\mathrm{s}$ cross-sections in nuclear collisions at the LHC. The rate for electromagnetic dissociation of $0n0n$ $\gamma +A\to \mathrm{j}\mathrm{e}\mathrm{t}\mathrm{s}$ events is also measured and compared to the analogous result from collisions with single-sided neutron emission. These comparisons support the hypothesis that $\gamma +A\to \mathrm{j}\mathrm{e}\mathrm{t}\mathrm{s}$ events without forward neutron emission select a more peripheral class of $\gamma +A$ collisions.