Corrected Delta_{recoil} distribution of recoil jets with R=0.4 measured for p-Pb collisions at sqrt{s_{NN}} = 5.02 TeV with event activity V0A 0-20%.

Corrected Delta_{recoil} distribution of recoil jets with R=0.4 measured for p-Pb collisions at sqrt{s_{NN}} = 5.02 TeV with event activity V0A 50-100%.

Corrected Delta_{recoil} distribution of recoil jets with R=0.2 measured for p-Pb collisions at sqrt{s_{NN}} = 5.02 TeV without imposing event activity bias.

Corrected Delta_{recoil} distribution of recoil jets with R=0.2 measured for p-Pb collisions at sqrt{s_{NN}} = 5.02 TeV with event activity ZNA 0-20%.

Corrected Delta_{recoil} distribution of recoil jets with R=0.2 measured for p-Pb collisions at sqrt{s_{NN}} = 5.02 TeV with event activity ZNA 50-100%.

Corrected Delta_{recoil} distribution of recoil jets with R=0.2 measured for p-Pb collisions at sqrt{s_{NN}} = 5.02 TeV with event activity V0A 0-20%.

Corrected Delta_{recoil} distribution of recoil jets with R=0.2 measured for p-Pb collisions at sqrt{s_{NN}} = 5.02 TeV with event activity V0A 50-100%.

Ratio of event activity biased Delta_{recoil} distributions corresponding to recoil jets with R=0.4.

Ratio of event activity biased Delta_{recoil} distributions corresponding to recoil jets with R=0.4.

Ratio of event activity biased Delta_{recoil} distributions corresponding to recoil jets with R=0.2.

Ratio of event activity biased Delta_{recoil} distributions corresponding to recoil jets with R=0.2.

Expected and observed 95 percent CL upper limits on BR(H to etau) for each individual category and combined from collinear mass fit analysis

Summary of the observed and expected upper limits at the 95percent CL and the best fit branching fractions in percent for the H->mutau and H->etau processes, for the main analysis (BDT fit) and the cross check (Mcol fit) method.

95 percent CL observed upper limit on the Yukawa couplings for the main analysis (BDT fit) and the cross check (Mcol fit) method

Centrality dependence of nu_dyn.

Centrality dependence of nu_dyn.

Centrality dependence of nu_dyn.

Differential cross section of J/psi mesons from b hadrons as a function of dimuon pT in pp and PbPb collisions. The PbPb cross sections are normalised by TAA for direct comparison. Global uncertainties arise from the integrated luminosity uncertainty in pp collisions, and the number of minimum bias events and TAA uncertainties for PbPb collisions.

Differential cross section of prompt J/psi mesons as a function of dimuon rapidty in pp and PbPb collisions. The PbPb cross sections are normalised by TAA for direct comparison. Global uncertainties arise from the integrated luminosity uncertainty in pp collisions, and the number of minimum bias events and TAA uncertainties for PbPb collisions.

Differential cross section of J/psi mesons from b hadrons as a function of dimuon rapidty in pp and PbPb collisions. The PbPb cross sections are normalised by TAA for direct comparison. Global uncertainties arise from the integrated luminosity uncertainty in pp collisions, and the number of minimum bias events and TAA uncertainties for PbPb collisions.

Nuclear modification factor of prompt J/psi mesons as a function of dimuon rapidity. Global uncertainties arise from the integrated luminosity uncertainty of the pp data, and the number of minimum bias events and TAA uncertainties of the PbPb data.

Nuclear modification factor of prompt J/psi mesons as a function of collision centrality. Global uncertainties arise from the full pp statistical and systematic uncertainties (including integrated luminosity uncertainty), and the number of minimum bias events uncertainty of the PbPb data.

Nuclear modification factor of prompt J/psi mesons as a function of dimuon pT. Global uncertainties arise from the integrated luminosity uncertainty of the pp data, and the number of minimum bias events and TAA uncertainties of the PbPb data.

Nuclear modification factor of prompt J/psi mesons as a function of dimuon pT in the mid-rapidity interval. Global uncertainties arise from the integrated luminosity uncertainty of the pp data, and the number of minimum bias events and TAA uncertainties of the PbPb data.

Nuclear modification factor of prompt J/psi mesons as a function of dimuon pT in the most forward rapidity interval. Global uncertainties arise from the integrated luminosity uncertainty of the pp data, and the number of minimum bias events and TAA uncertainties of the PbPb data.

Nuclear modification factor of prompt J/psi mesons as a function of collision centrality in the mid- and most forward rapidity intervals. Global uncertainties arise from the full pp statistical and systematic uncertainties (including integrated luminosity uncertainty), and the number of minimum bias events uncertainty of the PbPb data.

Nuclear modification factor of prompt J/psi mesons as a function of pT in three centrality bins. Global uncertainties arise from the integrated luminosity uncertainty of the pp data, and the number of minimum bias events and TAA uncertainties of the PbPb data.

Nuclear modification factor of prompt J/psi mesons as a function of collision centrality in the most forward rapidity range at moderate and high pT. Global uncertainties arise from the full pp statistical and systematic uncertainties (including integrated luminosity uncertainty), and the number of minimum bias events uncertainty of the PbPb data.

Nuclear modification factor of prompt J/psi mesons as a function of collision centrality in the mid-rapidity range. Global uncertainties arise from the full pp statistical and systematic uncertainties (including integrated luminosity uncertainty), and the number of minimum bias events uncertainty of the PbPb data.

Nuclear modification factor of prompt psi(2S) mesons as a function of collision centrality in the mid-rapidity range. Global uncertainties arise from the full pp statistical and systematic uncertainties (including integrated luminosity uncertainty), and the number of minimum bias events uncertainty of the PbPb data.

95% CL intervals on the nuclear modification factor of prompt psi(2S) mesons as a function of collision centrality in the mid-rapidity range. Global uncertainties arise from the full pp statistical and systematic uncertainties (including integrated luminosity uncertainty), and the number of minimum bias events uncertainty of the PbPb data.

Nuclear modification factor of prompt J/psi and psi(2S) mesons as a function of dimuon pT in the mid-rapidity range. Global uncertainties arise from the integrated luminosity uncertainty of the pp data, and the number of minimum bias events and TAA uncertainties of the PbPb data.

Nuclear modification factor of prompt J/psi mesons as a function of collision centrality in the forward rapidity range. Global uncertainties arise from the full pp statistical and systematic uncertainties (including integrated luminosity uncertainty), and the number of minimum bias events uncertainty of the PbPb data.

Nuclear modification factor of prompt psi(2S) mesons as a function of collision centrality in the forward rapidity range. Global uncertainties arise from the full pp statistical and systematic uncertainties (including integrated luminosity uncertainty), and the number of minimum bias events uncertainty of the PbPb data.

95% CL intervals on the nuclear modification factor of prompt psi(2S) mesons as a function of collision centrality in the forward rapidity range. Global uncertainties arise from the full pp statistical and systematic uncertainties (including integrated luminosity uncertainty), and the number of minimum bias events uncertainty of the PbPb data.

Nuclear modification factor of prompt J/psi mesons as a function of dimuon pT in the forward rapidity range. Global uncertainties arise from the integrated luminosity uncertainty of the pp data, and the number of minimum bias events and TAA uncertainties of the PbPb data.

Nuclear modification factor of prompt psi(2S) mesons as a function of dimuon pT in the forward rapidity range. Global uncertainties arise from the integrated luminosity uncertainty of the pp data, and the number of minimum bias events and TAA uncertainties of the PbPb data.

95% CL intervals on the nuclear modification factor of prompt psi(2S) mesons as a function of dimuon pT in the forward rapidity range. Global uncertainties arise from the integrated luminosity uncertainty of the pp data, and the number of minimum bias events and TAA uncertainties of the PbPb data.

Nuclear modification factor of nonprompt J/psi mesons as a function of dimuon rapidity. Global uncertainties arise from the integrated luminosity uncertainty of the pp data, and the number of minimum bias events and TAA uncertainties of the PbPb data.

Nuclear modification factor of nonprompt J/psi mesons as a function of collision centrality. Global uncertainties arise from the full pp statistical and systematic uncertainties (including integrated luminosity uncertainty), and the number of minimum bias events uncertainty of the PbPb data.

Nuclear modification factor of nonprompt J/psi mesons as a function of dimuon pT. Global uncertainties arise from the integrated luminosity uncertainty of the pp data, and the number of minimum bias events and TAA uncertainties of the PbPb data.

Nuclear modification factor of nonprompt J/psi mesons as a function of dimuon pT in the mid-rapidity interval. Global uncertainties arise from the integrated luminosity uncertainty of the pp data, and the number of minimum bias events and TAA uncertainties of the PbPb data.

Nuclear modification factor of nonprompt J/psi mesons as a function of dimuon pT in the most forward rapidity interval. Global uncertainties arise from the integrated luminosity uncertainty of the pp data, and the number of minimum bias events and TAA uncertainties of the PbPb data.

Nuclear modification factor of nonprompt J/psi mesons as a function of collision centrality in the mid- and most forward rapidity intervals. Global uncertainties arise from the full pp statistical and systematic uncertainties (including integrated luminosity uncertainty), and the number of minimum bias events uncertainty of the PbPb data.

Nuclear modification factor of nonprompt J/psi mesons as a function of pT in three centrality bins. Global uncertainties arise from the integrated luminosity uncertainty of the pp data, and the number of minimum bias events and TAA uncertainties of the PbPb data.

Nuclear modification factor of nonprompt J/psi mesons as a function of collision centrality in the most forward rapidity range at moderate and high pT. Global uncertainties arise from the full pp statistical and systematic uncertainties (including integrated luminosity uncertainty), and the number of minimum bias events uncertainty of the PbPb data.

Figure 8. Gluino pair production cross section.

Table 1. Post-fit yields for the background-only fit, observed data, and expected yields for mgluino = 1600 GeV in each search bin.

The $\Lambda_{\rm {c}}^{+}$/${\rm D}^{0}$ ratio measured in p-Pb collisions at $\sqrt{s_{\rm {NN}}} = 5.02$ TeV in the rapidity interval $-0.96 \lt y \lt 0.04$ as a function of $p_{\rm {T}}$.

The $\Lambda_{\rm {c}}^{+}$/${\rm D}^{0}$ ratio measured in pp collisions at $\sqrt{s} = 7$ TeV in the transverse momentum interval $ 1 \lt p_{\rm T} \lt 8$ GeV/c and in the rapidity interval $|y|<0.5$.

The $\Lambda_{\rm {c}}^{+}$/${\rm D}^{0}$ ratio measured in p-Pb collisions at $\sqrt{s_{\rm {NN}}} = 5.02$ TeV in the transverse momentum interval $2 \lt p_{\rm T} \lt 12$ GeV/c and in the rapidity interval $-0.96 \lt y \lt 0.04$.

The nuclear modification factor $R_\mathrm{pPb}$ of prompt $\Lambda_{\rm {c}}^{+}$ baryons in p-Pb collisions at $\sqrt{s_{\rm {NN}}} = 5.02$ TeV in the rapidity interval $ -0.96\lt y \lt 0.04$.

Measured signal cross section for dielectron, dimuon and combined dilepton channels. The measurement is performed in a kinematic region defined by invariant masses $m_{ll}~>~50$ GeV, $m_{jj}~>~120$ GeV, and transverse momenta $p_{Tj}~>~25$ GeV, where $l$ denotes electrons and muons, and $j$ - quarks produced in the hard interaction.

Distributions of $p_{TZ}$ in data and total SM background, EW Zjj signal and two ATGC scenarios in the dimuon channel

Distributions of $p_{TZ}$ in data and total SM background, EW Zjj signal and two ATGC scenarios in the dielectron channel

Distributions of $m_{jj}$ in data and total SM background and EW Zjj signal in the dimuon channel. Kinematic region is defined by invariant masses $m_{ll}~>~50$ GeV, $m_{jj}~>~120$ GeV, and transverse momenta $p_{Tj}~>~25$ GeV, where $l$ denotes electrons and muons, and $j$ - quarks produced in the hard interaction.

Distributions of $m_{jj}$ in data and total SM background and EW Zjj signal in the dimuon channel. Kinematic region is defined by invariant masses $m_{ll}~>~50$ GeV, $m_{jj}~>~120$ GeV, and transverse momenta $p_{Tj}~>~25$ GeV, where $l$ denotes electrons and muons, and $j$ - quarks produced in the hard interaction.

Distributions of the transformed BDT discriminant in data and total SM background and EW Zjj signal in the dimuon channel. Kinematic region is defined by invariant masses $m_{ll}~>~50$ GeV, $m_{jj}~>~120$ GeV, and transverse momenta $p_{Tj}~>~25$ GeV, where $l$ denotes electrons and muons, and $j$ - quarks produced in the hard interaction.

Distributions of the transformed BDT discriminant in data and total SM background and EW Zjj signal in the dimuon channel. Kinematic region is defined by invariant masses $m_{ll}~>~50$ GeV, $m_{jj}~>~120$ GeV, and transverse momenta $p_{Tj}~>~25$ GeV, where $l$ denotes electrons and muons, and $j$ - quarks produced in the hard interaction.

Efficiency of a gap activity veto in dielectron and dimuon events with BDT > 0.92, as a function of the additional jet $p_T$ for data, MC expectations with only DY events, including signal with the PYTHIA PS model, or the HERWIG++ PS model.

Efficiency of a gap activity veto in dielectron and dimuon events with BDT > 0.92, as a function of total $H_T$ of additional jets for data, MC expectations with only DY events, including signal with the PYTHIA PS model, or the HERWIG++ PS model.

Efficiency of a gap activity veto in dielectron and dimuon events with BDT > 0.92, as a function of total soft $H_T$ for data, MC expectations with only DY events, including signal with the PYTHIA PS model, or the HERWIG++ PS model.

Efficiency of a gap activity veto in dielectron and dimuon events with BDT > 0.92, as a function of the leading soft track-jet $p_T$ for data, MC expectations with only DY events, including signal with the PYTHIA PS model, or the HERWIG++ PS model.

The $\varepsilon_{\text{reco}}$ values as a function of $E_{g}$, for $\tilde{g}$ R-hadrons that stop in the EB or HB, in the MC simulation, for the calorimeter search. The $\varepsilon_{\text{reco}}$ values are plotted for the two-body gluino decay, when $m_{\tilde{g}}$ is 1200 GeV.

The $\varepsilon_{\text{reco}}$ values as a function of $E_{g}$, for $\tilde{g}$ R-hadrons that stop in the EB or HB, in the MC simulation, for the calorimeter search. The $\varepsilon_{\text{reco}}$ values are plotted for the two-body gluino decay, when $m_{\tilde{g}}$ is 1800 GeV.

The $\varepsilon_{\text{reco}}$ values as a function of $E_{t}$, for $\tilde{t}$ R-hadrons that stop in the EB or HB, in the MC simulation, for the calorimeter search. The $\varepsilon_{\text{reco}}$ values are plotted for the two-body top squark decays, when $m_{\tilde{t}}$ is 400 GeV.

The $\varepsilon_{\text{reco}}$ values as a function of $E_{t}$, for $\tilde{t}$ R-hadrons that stop in the EB or HB, in the MC simulation, for the calorimeter search. The $\varepsilon_{\text{reco}}$ values are plotted for the two-body top squark decays, when $m_{\tilde{t}}$ is 600 GeV.

The $\varepsilon_{\text{reco}}$ values as a function of $E_{t}$, for $\tilde{t}$ R-hadrons that stop in the EB or HB, in the MC simulation, for the calorimeter search. The $\varepsilon_{\text{reco}}$ values are plotted for the two-body top squark decays, when $m_{\tilde{t}}$ is 1000 GeV.

The $\varepsilon_{\text{reco}}$ values as a function of $m_{\tilde{g}} - m_{\tilde{\chi}^{0}}$, for $\tilde{g}$ R-hadrons that stop in the EB or HB, in the MC simulation, for the calorimeter search. The $\varepsilon_{\text{reco}}$ values are plotted for the three-body gluino decay, when $m_{\tilde{g}}$ is 800 and 1000 GeV.

The $\varepsilon_{\text{reco}}$ values as a function of $m_{\tilde{g}} - m_{\tilde{\chi}^{0}}$, for $\tilde{g}$ R-hadrons that stop in the EB or HB, in the MC simulation, for the calorimeter search. The $\varepsilon_{\text{reco}}$ values are plotted for the three-body gluino decay, when $m_{\tilde{g}}$ is 1800 GeV.

The background extrapolation for the muon search. The integral of the fit function to $\Delta t_{DT}$ with the sum of two Gaussian distributions and a Crystal Ball function, for $\Delta t_{DT}$>−20 ns, is plotted as a function of the lower $\Delta t_{RPC}$ selection, for 2015 and 2016 data. The uncertainties correspond to when the fit function parameters are varied by one standard deviation.

The 95% CL upper limits on $\mathcal{B}\sigma$ for gluino pair production, using the cloud model of R-hadron interactions, as a function of lifetime, for combined 2015 and 2016 data for the calorimeter search. We show gluinos that undergo a two-body decay. The discontinuous structure observed between $10^{-7}$ and $10^{-5}$ s is due to the increase of the number of observed events in the search window as the lifetime increases.

The 95% CL upper limits on $\mathcal{B}\sigma$ for top squark pair production, using the cloud model of R-hadron interactions, as a function of lifetime, for combined 2015 and 2016 data for the calorimeter search. We show top squarks that undergo a two-body decay. The discontinuous structure observed between $10^{-7}$ and $10^{-5}$ s is due to the increase of the number of observed events in the search window as the lifetime increases.

The 95% CL upper limits on $\mathcal{B}\sigma$ for gluino pair production, using the cloud model of R-hadron interactions, as a function of lifetime, for combined 2015 and 2016 data for the calorimeter search. We show gluinos that undergo a three-body decay. The discontinuous structure observed between $10^{-7}$ and $10^{-5}$ s is due to the increase of the number of observed events in the search window as the lifetime increases.

The 95% CL upper limits on the gluino mass, using the cloud model of R-hadron interactions, as a function of lifetime, for combined 2015 and 2016 data for the calorimeter search. We show gluinos that undergo a two-body decay. The discontinuous structure observed between $10^{-7}$ and $10^{-5}$ s is due to the increase of the number of observed events in the search window as the lifetime increases.

The 95% CL upper limits on the top squark mass, using the cloud model of R-hadron interactions, as a function of lifetime, for combined 2015 and 2016 data for the calorimeter search. We show top squarks that undergo a two-body decay. The discontinuous structure observed between $10^{-7}$ and $10^{-5}$ s is due to the increase of the number of observed events in the search window as the lifetime increases.

The 95% CL upper limits on the gluino mass, using the cloud model of R-hadron interactions, as a function of lifetime, for combined 2015 and 2016 data for the calorimeter search. We show gluinos that undergo a three-body decay. The discontinuous structure observed between $10^{-7}$ and $10^{-5}$ s is due to the increase of the number of observed events in the search window as the lifetime increases.

The 95% CL upper limits in the neutralino mass vs.~gluino mass plane, for lifetimes between 10 $\mu$s and 1000 s, for combined 2015 and 2016 data for the calorimeter search. The mostly triangular region shows the excluded observed region. We show gluinos that undergo a two-body decay.

The 95% CL upper limits in the neutralino mass vs.~gluino mass plane, for lifetimes between 10 $\mu$s and 1000 s, for combined 2015 and 2016 data for the calorimeter search. The mostly triangular region shows the excluded expected region. We show gluinos that undergo a two-body decay.

The 95% CL upper limits in the neutralino mass vs.~gluino mass plane, for lifetimes between 10 $\mu$s and 1000 s, for combined 2015 and 2016 data for the calorimeter search. The mostly triangular region shows the excluded expected +1 s.d. region. We show gluinos that undergo a two-body decay.

The 95% CL upper limits in the neutralino mass vs.~gluino mass plane, for lifetimes between 10 $\mu$s and 1000 s, for combined 2015 and 2016 data for the calorimeter search. The mostly triangular region shows the excluded expected -1 s.d. region. We show gluinos that undergo a two-body decay.

The 95% CL upper limits in the neutralino mass vs.~top squark mass plane, for lifetimes between 10 $\mu$s and 1000 s, for combined 2015 and 2016 data for the calorimeter search. The mostly triangular region shows the excluded observed region. We show top squarks that undergo a two-body decay.

The 95% CL upper limits in the neutralino mass vs.~top squark mass plane, for lifetimes between 10 $\mu$s and 1000 s, for combined 2015 and 2016 data for the calorimeter search. The mostly triangular region shows the excluded expected region. We show top squarks that undergo a two-body decay.

The 95% CL upper limits in the neutralino mass vs.~top squark mass plane, for lifetimes between 10 $\mu$s and 1000 s, for combined 2015 and 2016 data for the calorimeter search. The mostly triangular region shows the excluded expected +1 s.d. region. We show top squarks that undergo a two-body decay.

The 95% CL upper limits in the neutralino mass vs.~top squark mass plane, for lifetimes between 10 $\mu$s and 1000 s, for combined 2015 and 2016 data for the calorimeter search. The mostly triangular region shows the excluded expected -1 s.d. region. We show top squarks that undergo a two-body decay.

The 95% CL upper limits in the neutralino mass vs.~gluino mass plane, for lifetimes between 10 $\mu$s and 1000 s, for combined 2015 and 2016 data for the calorimeter search. The mostly triangular region shows the excluded observed region. We show gluinos that undergo a three-body decay.

The 95% CL upper limits in the neutralino mass vs.~gluino mass plane, for lifetimes between 10 $\mu$s and 1000 s, for combined 2015 and 2016 data for the calorimeter search. The mostly triangular region shows the excluded expected region. We show gluinos that undergo a three-body decay.

The 95% CL upper limits in the neutralino mass vs.~gluino mass plane, for lifetimes between 10 $\mu$s and 1000 s, for combined 2015 and 2016 data for the calorimeter search. The mostly triangular region shows the excluded expected +1 s.d. region. We show gluinos that undergo a three-body decay.

The 95% CL upper limits in the neutralino mass vs.~gluino mass plane, for lifetimes between 10 $\mu$s and 1000 s, for combined 2015 and 2016 data for the calorimeter search. The mostly triangular region shows the excluded expected -1 s.d. region. We show gluinos that undergo a three-body decay.

The 95% CL upper limits on $\mathcal{B}\sigma$ for 1000 GeV gluino pair production as a function of lifetime, for combined 2015 and 2016 data for the muon search.

The 95% CL upper limits on $\mathcal{B}\sigma$ for 400 GeV MCHAMP pair production as a function of lifetime, for combined 2015 and 2016 data for the muon search.

95% CL upper limits on $\mathcal{B}\sigma$ for gluino pair production as a function of mass, for lifetimes between 10 $\mu$s and 1000 s, for combined 2015 and 2016 data for the muon search. The theory curves assume $\mathcal{B}=100\%$.

95% CL upper limits on $\mathcal{B}\sigma$ for MCHAMP pair production as a function of mass, for lifetimes between 10 $\mu$s and 1000 s, for combined 2015 and 2016 data for the muon search. The theory curves assume $\mathcal{B}=100\%$.

$\xi^\mathrm{jet}$ distributions for jets associated with an isolated photon in pp and 0-10% centrality PbPb collisions. The resolutions of the measured jet energy and azimuthal angle in pp are smeared to match those in the PbPb sample.

PbPb / pp ratio of $\xi^\mathrm{jet}$ distributions for 50-100% centrality collisions. The resolutions of the measured jet energy and azimuthal angle in pp are smeared to match those in the PbPb sample.

PbPb / pp ratio of $\xi^\mathrm{jet}$ distributions for 30-50% centrality collisions. The resolutions of the measured jet energy and azimuthal angle in pp are smeared to match those in the PbPb sample.

PbPb / pp ratio of $\xi^\mathrm{jet}$ distributions for 10-30% centrality collisions. The resolutions of the measured jet energy and azimuthal angle in pp are smeared to match those in the PbPb sample.

PbPb / pp ratio of $\xi^\mathrm{jet}$ distributions for 0-10% centrality collisions. The resolutions of the measured jet energy and azimuthal angle in pp are smeared to match those in the PbPb sample.

$\xi^\gamma_{\mathrm{T}}$ distributions for jets associated with an isolated photon in pp and 50-100% centrality PbPb collisions. The resolutions of the measured jet energy and azimuthal angle in pp are smeared to match those in the PbPb sample.

$\xi^\gamma_{\mathrm{T}}$ distributions for jets associated with an isolated photon in pp and 30-50% centrality PbPb collisions. The resolutions of the measured jet energy and azimuthal angle in pp are smeared to match those in the PbPb sample.

$\xi^\gamma_{\mathrm{T}}$ distributions for jets associated with an isolated photon in pp and 10-30% centrality PbPb collisions. The resolutions of the measured jet energy and azimuthal angle in pp are smeared to match those in the PbPb sample.

$\xi^\gamma_{\mathrm{T}}$ distributions for jets associated with an isolated photon in pp and 0-10% centrality PbPb collisions. The resolutions of the measured jet energy and azimuthal angle in pp are smeared to match those in the PbPb sample.

PbPb / pp ratio of $\xi^\gamma_{\mathrm{T}}$ distributions for 50-100% centrality collisions. The resolutions of the measured jet energy and azimuthal angle in pp are smeared to match those in the PbPb sample.

PbPb / pp ratio of $\xi^\gamma_{\mathrm{T}}$ distributions for 30-50% centrality collisions. The resolutions of the measured jet energy and azimuthal angle in pp are smeared to match those in the PbPb sample.

PbPb / pp ratio of $\xi^\gamma_{\mathrm{T}}$ distributions for 10-30% centrality collisions. The resolutions of the measured jet energy and azimuthal angle in pp are smeared to match those in the PbPb sample.

PbPb / pp ratio of $\xi^\gamma_{\mathrm{T}}$ distributions for 0-10% centrality collisions. The resolutions of the measured jet energy and azimuthal angle in pp are smeared to match those in the PbPb sample.