[{"nid":"11785","nid_1":"13443","title":"First measurement of $\\mathbf{\\rm \u039e_{\\rm c}^{0}}$ production in $\\mathbf{Pb}-\\mathbf{Pb}$ collisions at $\\mathbf{\\sqrt{\\textit{s}_{\\rm NN}}}$ = 5.02 TeV","field_draft_arxiv":"\u003Ca href=\u0022https:\/\/arxiv.org\/abs\/2607.17903\u0022\u003Ehttps:\/\/arxiv.org\/abs\/2607.17903\u003C\/a\u003E","field_paper_abstract":"\u003Cp\u003EThe ALICE Collaboration reports the first measurement of the production of prompt $\u039e_{\\mathrm c}^{0}$ baryons in nucleus$-$nucleus collisions by analyzing data from $\\mathrm{Pb}-\\mathrm{Pb}$ collisions at $\\sqrt{s_{\\mathrm{NN}}}~=5.02~\\mathrm{TeV}$. The production and transverse-momentum ($p_{\\mathrm T}$) differential spectra of $\u039e_{\\mathrm c}^{0}$ are particularly sensitive to the hadronization process and to strangeness production in the quark--gluon plasma formed in high-energy heavy-ion collisions. The $\u039e_{\\mathrm c}^{0}$ baryons are reconstructed at midrapidity ($|y|\u0026lt;~0.5$) in the transverse-momentum intervals $3\u0026lt;~p_{\\mathrm T}~\u0026lt;~12~\\mathrm{GeV}\/c$ and $4\u0026lt;~p_{\\mathrm T}~\u0026lt;~12~\\mathrm{GeV}\/c$ in the 0$-$10\\% and 30$-$50\\% centrality intervals, respectively. The nuclear modification factor ($R_{\\mathrm{AA}}$) reaches values up to 3 in the interval $3\u0026lt;~p_{\\mathrm T}~\u0026lt;~4~\\mathrm{GeV}\/c$, which is the largest value measured so far for charm hadrons. Model predictions are compatible with the measured $R_{\\mathrm{AA}}$, while, in the measured $p_{\\mathrm T}$ intervals, they underestimate the production yield as well as the measured $\u039e_{\\mathrm c}^{0}\/\\mathrm{D}^{0}$, $\u039e_{\\mathrm c}^{0}\/\u039b_{\\mathrm c}^{+}$, and $\u039e_{\\mathrm c}^{0}\/\\mathrm{D}^{+}_{\\mathrm s}$ yield ratios.\u003C\/p\u003E"},{"nid":"11831","nid_1":"13402","title":"Multiplicity dependence of the size of the common hadron emission source in pp collisions at the LHC","field_draft_arxiv":"\u003Ca href=\u0022https:\/\/arxiv.org\/abs\/2606.28098\u0022\u003Ehttps:\/\/arxiv.org\/abs\/2606.28098\u003C\/a\u003E","field_paper_abstract":"\u003Cp\u003EFemtoscopic analysis can shed light on hadron production in pp collisions. In this paper, proton-proton correlations measured in collisions at $\\sqrt{s}=13.6$ TeV recorded with the ALICE detector at the LHC are presented. The analysis is based on the minimum bias dataset collected in 2022 following the upgrade of the ALICE detector and corresponds to an integrated luminosity of $19.3$ pb$^{-1}$. The increased integrated luminosity allows us, for the first time, to simultaneously measure the multiplicity and transverse-mass ($m_{\\rm T}$) dependence of the size of the hadron-emitting source. Precise knowledge of the femtoscopic source size in pp collisions is a crucial ingredient for using femtoscopy to study the residual strong interaction among stable and unstable hadrons at the LHC. In this light, the source radius was determined from the measured correlation functions by assuming several state-of-the-art models of the nucleon$-$nucleon interactions. The consistency among the extracted radii demonstrates the robustness of the measurement with respect to interaction model assumptions. A comparison to femtoscopic radii measured in Pb$-$Pb collisions at $\\sqrt{s}=5.02$ TeV reveals a markedly different multiplicity dependence in similar $m_{\\rm T}$ intervals, providing new insight into the system-size dependence of particle emission dynamics.\u003C\/p\u003E"},{"nid":"13027","nid_1":"13374","title":"Evidence for parton energy loss in oxygen$-$oxygen collisions at $\\mathbf{\\sqrt{s_{\\rm NN}}=5.36}$ TeV","field_draft_arxiv":"\u003Ca href=\u0022https:\/\/arxiv.org\/abs\/2606.19967\u0022\u003Ehttps:\/\/arxiv.org\/abs\/2606.19967\u003C\/a\u003E","field_paper_abstract":"\u003Cp\u003EUltra-relativistic heavy-ion collisions create a hot and dense medium of deconfined quarks and gluons, the quark$-$gluon plasma (QGP), in which parton energy loss (\u0022jet quenching\u0022) is a key probe of hot medium properties. While parton energy loss has been firmly established in large systems such as Pb$-$Pb and Au$-$Au collisions, no unambiguous direct evidence exists in smaller systems such as high-multiplicity p$-$Pb and pp collisions. To probe the onset of parton energy loss at intermediate system size, measurements of neutral-pion production are presented in this Letter for oxygen$-$oxygen (OO) and proton$-$oxygen (pO) collisions recorded with the ALICE detector in July 2025, relative to a pp baseline. The nuclear modification factor $R_{\\rm OO}$ is suppressed relative to unity with a transverse-momentum dependence similar to that observed in Pb$-$Pb collisions, consistent with a previous CMS measurement in OO collisions with charged particles. As $R_{\\rm OO}$ contains contributions from both cold and hot nuclear matter effects, $R_{\\rm pO}$ is also presented in order to constrain cold nuclear matter (CNM) contributions. $R_{\\rm pO}$ is found to be compatible with unity, indicating that CNM effects alone cannot account for the suppression observed in $R_{\\rm OO}$. Final-state effects are isolated using the measured double ratio $R_{\\rm OO} \\left\/ R_{\\rm pO}^2 \\right.$, which largely cancels CNM contributions and exhibits a significant suppression relative to expectations without energy loss at a $4.9\u03c3$ level. Theoretical models incorporating parton energy loss via different mechanisms predict a significant suppression of the $R_{\\rm OO} \\left\/ R_{\\rm pO}^2 \\right.$ relative to unity, consistent with the data. These findings establish parton energy loss in OO collisions, extending experimental evidence for jet quenching to the smallest nuclear system studied to date.\u003C\/p\u003E"},{"nid":"12743","nid_1":"13375","title":"Probing flavor effects in the QCD parton shower using $\\mathbf{{\\rm D}^0}$-tagged jet angularities in proton$-$proton collisions at $\\mathbf{ \\sqrt{s} = 5.02}$ TeV","field_draft_arxiv":"\u003Ca href=\u0022https:\/\/arxiv.org\/abs\/2606.20028\u0022\u003Ehttps:\/\/arxiv.org\/abs\/2606.20028\u003C\/a\u003E","field_paper_abstract":"\u003Cp\u003EThe ALICE Collaboration presents the first measurements of ${\\rm D}^0$-tagged jet angularities in proton$-$proton (pp) collisions at $\\sqrt{s} = 5.02$ TeV. Jet angularities are powerful substructure observables that characterize the angular and momentum distributions of particles within jets via tunable weighting parameters. Varying the angular parameter in jet angularities allows for a systematic probe of the sensitivity to collinear and soft radiation, enabling the study of flavor-dependent fragmentation and hadronization through comparisons of jets initiated by different partons. This paper reports ${\\rm D}^0$-tagged and inclusive (gluon-dominated) charged-particle jet angularities with a resolution parameter $R=0.4$ in the low jet transverse momentum range ($10 \u0026lt;~ p_{\\rm T}^{\\rm ch. \\, jet} \u0026lt;~ 20$ GeV\/$c$), where charm-quark mass effects are most significant. At low angular weight, which emphasizes collinear radiation, ${\\rm D}^0$-tagged jets exhibit smaller angularity values than inclusive jets. This provides evidence for the radiation suppression from massive quarks -- a phenomenon known as the QCD dead-cone effect. As the angular weight increases, giving more emphasis to wide-angle radiation, the difference between ${\\rm D}^0$-tagged and inclusive jet distributions decreases. This indicates that the modification is concentrated within the jet core rather than its edge. PYTHIA 8 simulations qualitatively reproduce both the angularity of ${\\rm D}^0$-tagged and inclusive charged-particle jets, but reproduce the ${\\rm D}^0$-tagged jet distributions better than those of inclusive jets, offering a powerful new constraint for models. These results provide insight into flavor-dependent fragmentation and establish an essential baseline for future studies of jet modifications in the quark-gluon plasma produced in heavy-ion collisions.\u003C\/p\u003E"},{"nid":"11783","nid_1":"13377","title":"Precision mass measurements of multistrange baryons and their antiparticles","field_draft_arxiv":"\u003Ca href=\u0022https:\/\/arxiv.org\/abs\/2606.20144\u0022\u003Ehttps:\/\/arxiv.org\/abs\/2606.20144\u003C\/a\u003E","field_paper_abstract":"\u003Cp\u003EThe $\u03a9^-$ baryon, composed of three strange quarks (sss), was predicted by the quark model and discovered in 1964, playing a pivotal role in establishing quarks as fundamental constituents of matter. Despite its importance, experimental knowledge of its mass remains limited, with the current world average relying on measurements performed more than four decades ago and lacking robust estimates of systematic uncertainties. This is notable given the central role of the $\u03a9^-$ mass, and alternatively that of the $\u039e^-$(dss), in lattice QCD calculations, where it is widely used to set the overall physical scale. Precise scale setting is essential for first-principles studies of quark confinement, chiral symmetry breaking, and stringent tests of the Standard Model. Here we report high-precision measurements of the masses of the $\u03a9^-$ and $\u039e^-$ baryons and their antiparticles, determined from invariant-mass reconstruction of their decay products in proton$-$proton collisions at the LHC. The analysis exploits the excellent tracking and particle-identification capabilities of the ALICE experiment, enabling accurate reconstruction of the displaced decay vertices characteristic of these short-lived particles. Each mass is measured with a fractional uncertainty of about 60 parts per million, for example $M_{\\bar\u03a9^+}=1672.558\\,\\pm\\,0.034\\,({\\rm stat.})\\,\\pm\\,0.102\\,({\\rm syst.})$ MeV\/$c^2$. The precisely known K$^0_{\\rm S}$ and $\u039b$ masses are used for calibration. These results establish new precision benchmarks in strange-baryon spectroscopy and enable stringent tests of Charge-Parity-Time invariance in the multistrange-hadron sector. Our measurement reduces the scale uncertainty in lattice QCD calculations, enabling for instance sub per mille precision for the hadronic vacuum-polarization contribution to the muon anomalous magnetic moment.\u003C\/p\u003E"}]