[{"nid":"11939","nid_1":"13335","title":"Exclusive dimuon production and coherent charmonium photoproduction at forward rapidity in ultra-peripheral Pb$-$Pb collisions at $\\mathbf{\\sqrt{s_{\\rm NN}}=5.36}$ TeV","field_draft_arxiv":"\u003Ca href=\u0022https:\/\/arxiv.org\/abs\/2605.13569\u0022\u003Ehttps:\/\/arxiv.org\/abs\/2605.13569\u003C\/a\u003E","field_paper_abstract":"\u003Cp\u003EThis Paper presents rapidity-differential measurements of coherent J\/$\u03c8$ and $\u03c8({\\rm 2S})$ photoproduction, as well as rapidity- and mass-differential measurements of exclusive dimuon production, in the forward rapidity region $-4 \u0026lt;~ y \u0026lt;~ -2.5$ in ultra-peripheral Pb$-$Pb collisions at $\\sqrt{s_{\\rm NN}}=5.36$ TeV using data recorded by the ALICE detector at the LHC in 2023, corresponding to an integrated luminosity of $\\mathcal{L} = 1170 \\pm 50~\u03bc{\\rm b}^{-1}$. The J\/$\u03c8$ and $\u03c8({\\rm 2S})$ results reveal the significant role of nuclear shadowing effects. The square root of the ratio of the measured quarkonium cross section to the impulse approximation prediction is about 0.76 for J\/$\u03c8$ and 0.71 for $\u03c8({\\rm 2S})$, at $y \\approx -3$, corresponding to typical Bjorken-$x$ values of $10^{-2}$. The exclusive dimuon results highlight the sensitivity of such measurements to precise modeling of the photon flux, particularly at impact parameters near the nuclear radius.\u003C\/p\u003E"},{"nid":"11787","nid_1":"13245","title":"$\\mathbf{\\textbf{K}^{0}_{\\textbf{S}}}-\\mathbf{\\textbf{K}^{0}_{\\textbf{S}}}$ femtoscopy in Pb$-$Pb collisions at $\\mathbf{\\sqrt{\\textit{s}_{\\rm NN}} = 5.02}$ TeV at the LHC","field_draft_arxiv":"\u003Ca href=\u0022https:\/\/arxiv.org\/abs\/2605.02321\u0022\u003Ehttps:\/\/arxiv.org\/abs\/2605.02321\u003C\/a\u003E","field_paper_abstract":"\u003Cp\u003EResults from a one-dimensional femtoscopic analysis of ${\\rm K}^{0}_{\\rm S}-{\\rm K}^{0}_{\\rm S}$ correlations in Pb$-$Pb collisions at the center-of-mass energy $\\sqrt{s_{\\mathrm{NN}}}~=~5.02$ TeV using data collected by the ALICE experiment at the LHC are presented. The source radius $R$ and correlation strength $\u03bb$ are studied as a function of centrality and pair-transverse momentum ($k_{\\rm T}$) to provide insight into the space-time structure and composition of the particle-emitting source. The observed trends of radii as a function of $k_{\\rm T}$ and centrality are consistent with the collective expansion of the system. Comparisons with measurements at $\\sqrt{s_{\\mathrm{NN}}}~=~2.76$ TeV by the ALICE Collaboration show agreement across multiplicities and $k_{\\rm T}$. Hydrokinetic model predictions match the most central collision results but deviate in peripheral events, potentially reflecting limitations in the model\u0027s description of peripheral collisions. A comparison with recent measurements at the same energy by the CMS Collaboration shows compatibility in both $R$ and $\u03bb$ within 1.3$\u03c3$. These results extend previous ${\\rm K}^{0}_{\\rm{S}}-{\\rm K}^{0}_{\\rm{S}}$ femtoscopy to a higher energy, providing a consistent baseline for future comparisons.\u003C\/p\u003E"},{"nid":"12687","nid_1":"13246","title":"Measurement of isolated-prompt photon$-$hadron correlations in Pb$-$Pb collisions at $\\mathbf{\\sqrt{\\textit{s}_{\\rm NN}} = }$ 5.02 TeV","field_draft_arxiv":"\u003Ca href=\u0022https:\/\/arxiv.org\/abs\/2605.02342\u0022\u003Ehttps:\/\/arxiv.org\/abs\/2605.02342\u003C\/a\u003E","field_paper_abstract":"\u003Cp\u003EThe ALICE Collaboration has measured the azimuthal correlation between trigger isolated-prompt photons and associated charged hadrons in Pb$-$Pb collisions at the CERN LHC, at a centre-of-mass energy per nucleon pair of $\\sqrt{\\textit{s}_{\\rm NN}} = 5.02$ TeV. The trigger isolated-prompt photons are measured in the transverse-momentum range $18\u0026lt;~ p_{\\rm T}^\u03b3 \u0026lt;~ 40$ GeV\/$c$ and pseudorapidity range $|\u03b7^\u03b3| \u0026lt;~0.67$. The isolation selection is based on a charged particle isolation momentum threshold $p_{\\rm T}^{\\rm iso, ch} = 1.5$ GeV\/$c$ within a cone of radius $R=0.2$. The associated charged particles are measured in the transverse-momentum ranges $p_{\\rm T}^{\\rm h} \u0026gt; 1.8$ GeV\/$c$ and pseudorapidity $|\u03b7^{\\rm h}| \u0026lt;~0.9$. The yield D$(z_{\\rm T})$ of associated hadrons per trigger, with $z_{\\rm T} = p_{\\rm T}^{\\rm h}\/p_{\\rm T}^\u03b3$, is measured in three Pb$-$Pb collision centrality classes: central (0$-$30%), semicentral (30$-$50%), and peripheral (50$-$90%). An approximation to the standard $I_{\\rm AA}$ is computed from the D$(z_{\\rm T})$ conditional yields, using NLO pQCD predictions as pp reference. A strong suppression of this ratio is observed in central collisions compared to peripheral collisions. The result extends to a lower $p_{\\rm T}^\u03b3$ relative to those reported in previously published Pb$-$Pb collisions measurements at $\\sqrt{s_{\\rm NN}}=5.02$ TeV. The measurement is compared to NLO pQCD calculations that include energy loss, and to the CoLBT-hydro model. The results from central collisions are also compared with measurements of jets correlated with isolated-prompt photons and of hadrons correlated with Z$^0$ bosons, both reported by the CMS Collaboration at the LHC, as well as with direct photon$-$hadron correlation measurements reported by the PHENIX and STAR Collaborations at RHIC.\u003C\/p\u003E"},{"nid":"12398","nid_1":"13215","title":"Multiplicity dependence of prompt and non-prompt J\/$\u03c8$ production at midrapidity in pp collisions at $\\sqrt{s} = 13$ TeV","field_draft_arxiv":"\u003Ca href=\u0022https:\/\/arxiv.org\/abs\/2604.07968\u0022\u003Ehttps:\/\/arxiv.org\/abs\/2604.07968\u003C\/a\u003E","field_paper_abstract":"\u003Cp\u003EThe yields of prompt and non-prompt J\/$\u03c8$ and the fraction of non-prompt J\/$\u03c8$ are measured at midrapidity ($|y| \u0026lt;~ 0.9$) via the dielectron decay channel as a function of the midrapidity charged-particle multiplicity ($|\u03b7| \u0026lt;~ 0.9$) in pp collisions at $\\sqrt{s} = 13$ TeV. The J\/$\u03c8$ yields and the multiplicity are normalized by their average value in inelastic collisions. The multiplicity-dependent yield ratio between prompt J\/$\u03c8$ and D$^0$ is reported. The multiplicity is further divided into three azimuthal regions with respect to the J\/$\u03c8$ momentum: toward the J\/$\u03c8$ emission direction, transverse, or opposite to it. A stronger-than-linear increase of the self-normalized yields is observed for both prompt and non-prompt J\/$\u03c8$ production, with similar trends. This behaviour is also observed in the toward region, while a weaker increase is observed in the transverse and away regions.\u003C\/p\u003E"},{"nid":"8431","nid_1":"13213","title":"Wave-Function Femtometry: Hypertriton - The Ultimate Halo Nucleus","field_draft_arxiv":"\u003Ca href=\u0022https:\/\/arxiv.org\/abs\/2604.07949\u0022\u003Ehttps:\/\/arxiv.org\/abs\/2604.07949\u003C\/a\u003E","field_paper_abstract":"\u003Cp\u003EThe interaction between nucleons and hyperons - baryons containing a strange quark - is key to understanding the properties of dense nuclear matter, such as that expected in the interior of neutron stars. Direct scattering experiments are hindered by the short lifetime of hyperons, prompting the study of hypernuclei - bound states of nucleons and hyperons - as an alternative approach. The lightest known hypernucleus, the hypertriton ($^3_\u039b$H), is a weakly bound state composed of a proton, a neutron and a $\u039b$ hyperon, and is believed to exhibit a halo-like structure with the $\u039b$ being loosely bound to a deuteron core. Based on the first measurement of hypertriton production in proton-proton collisions at the CERN Large Hadron Collider (LHC), its halo structure is confirmed. A successful description of the hypertriton production yield within the nuclear coalescence framework enables an estimation of the $\u039b$ separation from the deuteron core as $9.54^{+2.67}_{-1.11}$ fm.\u003C\/p\u003E\n"}]