10 Search Results

The transverse momentum spectra and integrated yields of anti-$$Σ$$ hyperons ($$\overline{\Sigma}^{\pm}$$) have been measured in and collisions at $$\sqrt{s_{\textrm{NN}}} = 5.02$$ TeV with the ALICE experiment. Measurements are performed via the newly accessed decay channel $$\overline{\Sigma}^{\pm}$$ → $$\bar{\textrm{n}}π^±$$. A new method of antineutron reconstruction with the PHOS electromagnetic spectrometer is developed and applied to this analysis. The p_T spectra of $$\overline{\Sigma}^{\pm}$$ are measured in the range 0.5 < p_T < 3 GeV/c and compared to predictions of the PYTHIA 8, DPMJET, PHOJET, EPOS LHC and EPOS4 models. The EPOS LHC and EPOS4 models provide the best descriptions of the measuredmore » spectra both in pp and p-Pb collisions, while models which do not account for multiparton interactions provide a considerably worse description at high p_T. The total yields of $$\overline{\Sigma }^{\pm }$$ in both pp and p-Pb collisions are compared to predictions of the Thermal-FIST model and dynamical models PYTHIA 8, DPMJET, PHOJET, EPOS LHC and EPOS4. All models reproduce the total yields in both colliding systems within uncertainties. The nuclear modification factors R_pPb for both $$\overline{\Sigma}^{+}$$ and $$\overline{\Sigma}^{-}$$ are evaluated and compared to those of protons, $$Λ$$ and $$Ξ$$ hyperons, and predictions of EPOS LHC and EPOS4 models. No deviations of R_pPb for $$\overline{\Sigma}^{\pm}$$ from the model predictions or measurements for other hadrons are found within uncertainties.« less

The first results of K*(892)^± production at midrapidity (|y| < 0.5) in pp collisions at $$\sqrt{s}$$= 13 TeV as a function of the event multiplicity are presented. The K*(892)^± has been reconstructed via its hadronic decay channel K*(892)^± → π^± + K$$^0_{\textrm{S}}$$ using the ALICE detector at the LHC. For each multiplicity class, the differential transverse momentum (p_T) spectrum, the mean transverse momentum ⟨p_T⟩, the p_T-integrated yield (dN/dy), and the ratio of the K*(892)^± to K$$^0_{\textrm{S}}$$ yields are reported. These are consistent with previous K*(892)⁰ resonance results with a higher level of precision. Comparisons with phenomenological models such as PYTHIA6,more » PYTHIA8, EPOS-LHC, and DIPSY are also discussed. For the first time, a significant K*(892)^±/K$$^0_{\textrm{S}}$$ suppression in pp collisions is observed at a 7σ level passing from low to high multiplicity events. The ratios of the p_T-differential yields of K*(892)^± and K$$^0_{\textrm{S}}$$ in high and low multiplicity events are also presented along with their double ratio. For p_T ≲ 2 GeV/c this double ratio persists below unity by more than 3σ suggesting that the suppression affects mainly low p_T resonances. The measured decreasing trend of the K*(892)^±/K$$^0_{\textrm{S}}$$ ratio with increasing multiplicity, which in heavy-ion collisions is typically attributed to the rescattering of decay particles of the short-lived resonances, is reproduced by the EPOS-LHC model without the use of hadronic afterburners.« less

In this letter, the first measurement of the femtoscopic correlation of protons and $Σ^+$ hyperons is presented and used to study the p–$Σ^+$ interaction. The measurement is performed with the ALICE detector in high-multiplicity triggered pp collisions at $$\sqrt{s}$$ = 13 TeV. The $Σ^+$ hyperons are reconstructed using a missing-mass approach in the decay channel to p + π⁰ with π⁰ → $γγ$, while both $Σ^+$ and protons are identified using a machine learning approach. These techniques result in a high reconstruction efficiency and purity, which allows the measurement of the p–$Σ^+$ correlation function for the first time. Thanks tomore » the high significance achieved in the p–$Σ^+$ correlation signal, it is possible to discriminate between the predictions of different models of the N–$$Σ$$ interaction and to accomplish a first determination of the p–$Σ^+$ scattering parameters.« less

Meson-baryon systems with strangeness content provide a unique laboratory for investigating the strong interaction and testing theoretical models of hadron structure and dynamics. In this work, the measured correlation functions for oppositely charged $$Ξ$$-K and $$Ξ$$ − 𝜋 pairs obtained in high-multiplicity pp collisions at $$\sqrt{𝑠}$$ = 13 TeV at the LHC are presented. For the first time, high-precision data on the $$Ξ$$-K interaction are delivered at small relative momenta. The scattering lengths, extracted via the Lednický–Lyuboshits expression of the pair wavefunction, indicate a repulsive and a shallow attractive strong interaction for the $$Ξ$$-K and $$Ξ$$ − 𝜋 systems, respectively.more » The $$Ξ$$(1620) and $$Ξ$$(1690) states are observed in the $$Ξ$$ − 𝜋 correlation function and their properties, mass and width, are determined. These measurements are in agreement with other available results. Such high-precision data can help refine the understanding of these resonant states, provide stronger constraints for chirally motivated potentials, and address the key challenge of describing the coupled-channel dynamics that may give rise to molecular configurations .« less

The dependence of f₀ (980) production on the final-state charged-particle multiplicity is reported for proton–proton (pp) collisions at the centre-of-mass energy, $$\mathbf{\sqrt{s}}$$ = 13 TeV. The production of (980) is measured with the ALICE detector via the decay channel in a midrapidity region of |y| < 0.5. The evolution of the integrated yields and mean transverse momentum of f₀ (980) as a function of charged-particle multiplicity measured in pp at $$\mathbf{\sqrt{s}}$$ = 13 TeV follows the trends observed in pp at $$\mathbf{\sqrt{s}}$$ = 5.02 TeV and in proton–lead (p–Pb) collisions at$$\mathbf{\sqrt{s_{NN}}}$$ = 5.02 TeV. Particle yield ratios of f₀ (980)more » to π^± and K* (892) are found to decrease with increasing charged-particle multiplicity. These particle ratios are compared with calculations from the canonical statistical thermal model as a function of charged-particle multiplicity. The thermal model calculations provide a better description of the decreasing trend of particle ratios when no strange or antistrange quark composition for f₀ (980) is assumed, which suggests that the data do not support significant hidden strangeness in the f₀ (980).« less

The first measurement at midrapidity (|y| < 0.5) of the production yield of the strange-charm baryons $$Ξ$$$^{+}_{c}$$ and $$Ξ$$$^{0}_{c}$$ as a function of transverse momentum (p_T) in different charged-particle multiplicity classes in proton-proton collisions at $$\sqrt{s}$$ = 13 TeV with the ALICE experiment at the LHC is reported. The $$Ξ$$$^{+}_{c}$$ baryon is reconstructed via the $$Ξ$$$^{+}_{c}$$ → $$Ξ$$^– π⁺π⁺ decay channel in the range 4 < p_T < 12 GeV/c, while the $$Ξ$$$^{0}_{c}$$ baryon is reconstructed via both the $$Ξ$$$^{0}_{c}$$ → $$Ξ$$^–π⁺ and $$Ξ$$$^{0}_{c}$$ → $$Ξ$$^–e⁺ν_e decay channels in the range 2 < p_T < 12 GeV/c. The baryon-to-meson ($$Ξ$$$^{0}_{c}$$⁺/D⁰)more » and the baryon-to-baryon ($$Ξ$$$^{0}_{c}$$⁺/Λ$$^{+}_{c}$$) production yield ratios show no significant dependence on multiplicity. In addition, the observed yield ratios are not described by theoretical predictions that model charm-quark fragmentation based on measurements at e⁺e⁻ and e⁻p colliders, indicating differences in the charm-baryon production mechanism in pp collisions. A comparison with different event generators and tunings, including different modelling of the hadronisation process, is also discussed.« less

Ultrarelativistic heavy-ion collisions produce a state of hot and dense strongly interacting QCD matter called quark-gluon plasma (QGP). On an event-by-event basis, the volume of the QGP in ultracentral collisions is mostly constant, while its total entropy can vary significantly due to quantum fluctuations, leading to variations in the temperature of the system. Exploiting this unique feature of ultracentral collisions allows for the interpretation of the correlation of the mean transverse momentum ($$\langle$$p_T$$\rangle$$) of produced charged hadrons and the number of charged hadrons as a measure for the speed of sound, c_s. This speed is related to the rate atmore » which compression waves travel in the QGP and is determined by fitting the relative increase in $$\langle$$p_T$$\rangle$$ with respect to the relative change in the average charged-particle density ($$\langle$$dN_ch/dη$$\rangle$$) measured at mid-rapidity. This study reports the event-average $$\langle$$p_T$$\rangle$$ of charged particles as well as the variance, skewness, and kurtosis of the event-by-event transverse momentum per charged particle ([p_T]) distribution in ultracentral Pb-Pb collisions at a center-of-mass energy of 5.02 TeV per nucleon pair using the ALICE detector. Different centrality estimators based on charged-particle multiplicity or the transverse energy of the event are used to select ultracentral collisions. By ensuring a pseudorapidity gap between the region used to define the centrality and the region used to perform the measurement, the influence of biases and their potential effects on the rise of the mean transverse momentum is tested. The measured c$$^{2}_{s}$$ is found to strongly depend on the exploited centrality estimator and ranges between 0.1146±0.0028 (stat.)±0.0065 (syst.) and 0.4374±0.0006 (stat.)±0.0184 (syst.) in natural units. The self-normalized variance shows a steep decrease towards ultracentral collisions, while the self-normalized skewness variables show a maximum, followed by a fast decrease. These non-Gaussian features are understood in terms of the vanishing of the impact-parameter fluctuations contributing to the event-to-event [p_T] distribution.« less

This work reports femtoscopic correlations of p – – p ($$\overline{p}$$ – – $$\overline{p}$$) and p – – d ($$\overline{p}$$ – – $$\overline{d}$$) pairs measured in Pb–Pb collisions at center-of-mass energy per nucleon $$\sqrt{s_{NN}}$$ = 5.02 TeV in the ALICE Collaboration. A fit to the measured proton-proton correlation functions allows one to extract the dependence of the nucleon femtoscopic radius of the particle-emitting source on the pair transverse mass (m_T) and on the average charge particle multiplicity $$\langle$$dN_ch/dη$$\rangle$$^1/3 for three centrality intervals (0–10%, 10 – – 30 %, 30 – – 50 %). In both cases, the expected power-law andmore » linear scalings are observed, respectively. The measured p–d correlations can be described by both two- and three-body calculations, indicating that the femtoscopy observable is not sensitive to the short-distance features of the dynamics of the p-(p-n) system, due to the large inter-particle distances in Pb–Pb collisions at the LHC. Indeed, in this study, the minimum measured femtoscopic source sizes for protons and deuterons have a minimum value at 2.73$$^{+0.05}_{–0.05}$$ and 3.10$$^{+1.04}_{–0.86}$$ fm, respectively, for the 30–50% centrality collisions. Moreover, the m_T-scaling obtained for the p–p and p–d systems is compatible within 1σ of the uncertainties. These findings provide new input for fundamental studies on the production of light (anti)nuclei under extreme conditions.« less

We report on a measurement of Spin Density Matrix Elements (SDMEs) in hard exclusive $$\rho ^0$$ meson muoproduction at COMPASS using 160 GeV/c polarised μ⁺ and μ^– beams impinging on a liquid hydrogen target. The measurement covers the kinematic range 5.0 GeV/c² < W < 17.0 GeV/c², 1.0 (GeV/c)² < $$\mathrm{Q}$$² < 10.0 (GeV/c)² and 0.01 (GeV/c)² < $$p_{\textrm{T}}^2$$ < 0.5 (GeV/c)². Here, W denotes the mass of the final hadronic system, $$\mathrm{Q}$$² the virtuality of the exchanged photon, and $$p_{\textrm{T}}$$ the transverse momentum of the $$\rho ^0$$ meson with respect to the virtual-photon direction. The measured non-zero SDMEs formore » the transitions of transversely polarised virtual photons to longitudinally polarised vector mesons ($$\gamma ^*_T \rightarrow V^{ }_L$$) indicate a violation of s-channel helicity conservation. Additionally, we observe a dominant contribution of natural-parity-exchange transitions and a very small contribution of unnatural-parity-exchange transitions, which is compatible with zero within experimental uncertainties. The results provide important input for modelling Generalised Parton Distributions (GPDs). In particular, they may allow one to evaluate in a model-dependent way the role of parton helicity-flip GPDs in exclusive $$\rho ^0$$ production.« less

The proposed new Electron–Ion Collider poses a technical and intellectual challenge for the detector design to accommodate the long-term diverse physics goals envisaged by the program. This requires a 4π detector system capable of reconstructing the energy and momentum of final state particles with high precision. The Electron-Ion Collider also requires identification of particles of different masses over a wide momentum range. A diverse spectrum of Particle IDentification detectors has been proposed. Of the four types of detectors for hadron identification, three are based on Ring Imaging Cherenkov Counter technologies, and one is realized by the Time of Flight method.more » The quest for a novel photocathode, sensitive in the far vacuum ultraviolet wavelength range and more robust than cesium iodide, motivated an R&D programme to explore nano-diamond (ND) based photocathodes, started by a collaboration between INFN and CNR Bari and INFN Trieste. Systematic measurements of the photoemission in different Ar:CH₄ and Ar:CO₂ gas mixtures with various types of ND powders and Hydrogenated ND (H-ND) powders are reported. A first study of the response of THGEMs coated with different photocathode materials is presented. Additionally, the progress of this R&D programme and the results obtained so far by these exploratory studies are described.« less