{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.104979.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1797451"}},{"@id":"https://doi.org/10.1103/PhysRevC.103.055201","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2021","description":"The first measurements of the scattering parameters of $\\Lambda$K pairs in all three charge combinations ($\\Lambda$K$^{+}$, $\\Lambda$K$^{-}$, and $\\Lambda\\mathrm{K^{0}_{S}}$) are presented.\nThe results are achieved through a femtoscopic analysis of $\\Lambda$K correlations in Pb--Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}$ = 2.76 TeV recorded by ALICE at the LHC.  \nThe femtoscopic correlations result from strong final-state interactions, and are fit with a parametrization allowing for both the characterization of the pair emission source and the measurement of the scattering parameters for the particle pairs.\nExtensive studies with the THERMINATOR 2 event generator provide a good description of the non-femtoscopic background, which results mainly from collective effects, with unprecedented precision.\nFurthermore, together with HIJING simulations, this model is used to account for contributions from residual correlations induced by feed-down from particle decays.\nThe extracted scattering parameters indicate that the strong force is repulsive in the $\\Lambda\\mathrm{K^{+}}$ interaction and attractive in the $\\Lambda\\mathrm{K^{-}}$ and $\\Lambda\\mathrm{K^{0}_{S}}$ interactions.\nThe results suggest an effect arising either from different quark--antiquark interactions between the pairs ($\\rm s\\overline{s}$ in $\\Lambda$K$^{+}$ and $\\rm u\\overline{u}$ in $\\Lambda$K$^{-}$) or from different net strangeness for each system (S=0 for $\\Lambda$K$^{+}$, and S=$-2$ for $\\Lambda$K$^{-}$).\nFinally, the $\\Lambda$K systems exhibit source radii larger than expected from extrapolation from identical particle femtoscopic studies.\nThis effect is interpreted as resulting from the separation in space--time of the single-particle $\\Lambda$ and K source distributions.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t1","@type":"Dataset","description":"Invariant mass distributions in the 0--10\\% centrality interval of (a) p$\\uppi^{-}$ pairs showing the $\\Lambda$ peak for V$^{0}$ candidates.","name":"Figure 1a"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t2","@type":"Dataset","description":"Invariant mass distributions in the 0--10\\% centrality interval of $\\uppi^{+}\\uppi^{-}$ pairs showing the $\\mathrm{K^{0}_{S}}$ peak for V$^{0}$ candidates.","name":"Figure 1b"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t3","@type":"Dataset","description":"Measured correlation function for the $\\Lambda\\mathrm{K^{+}}\\oplus\\overline{\\Lambda}\\mathrm{K^{-}}$ system in the 0--10\\% centrality interval.","name":"Figure 2a ALICE"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t4","@type":"Dataset","description":"THERMINATOR 2 simulation correlation function for the $\\Lambda\\mathrm{K^{+}}\\oplus\\overline{\\Lambda}\\mathrm{K^{-}}$ system in the 0--10\\% centrality interval.","name":"Figure 2a THERM"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t5","@type":"Dataset","description":"Measured correlation function for the $\\Lambda\\mathrm{K^{-}}\\oplus\\overline{\\Lambda}\\mathrm{K^{+}}$ system in the 0--10\\% centrality interval.","name":"Figure 2b ALICE"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t6","@type":"Dataset","description":"THERMINATOR 2 simulation correlation function for the $\\Lambda\\mathrm{K^{-}}\\oplus\\overline{\\Lambda}\\mathrm{K^{+}}$ system in the 0--10\\% centrality interval.","name":"Figure 2b THERM"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t7","@type":"Dataset","description":"Measured correlation function for the $\\Lambda\\mathrm{K^{0}_{S}}\\oplus\\overline{\\Lambda}\\mathrm{K^{0}_{S}}$ system in the 0--10\\% centrality interval.","name":"Figure 2c ALICE"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t8","@type":"Dataset","description":"THERMINATOR 2 simulation correlation function for the $\\Lambda\\mathrm{K^{0}_{S}}\\oplus\\overline{\\Lambda}\\mathrm{K^{0}_{S}}$ system in the 0--10\\% centrality interval.","name":"Figure 2c THERM"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t9","@type":"Dataset","description":"Measured correlation function for the $\\Lambda\\mathrm{K^{+}}\\oplus\\overline{\\Lambda}\\mathrm{K^{-}}$ system in the 10--30\\% centrality interval.","name":"Figure 2d ALICE"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t10","@type":"Dataset","description":"THERMINATOR 2 simulation correlation function for the $\\Lambda\\mathrm{K^{+}}\\oplus\\overline{\\Lambda}\\mathrm{K^{-}}$ system in the 10--30\\% centrality interval.","name":"Figure 2d THERM"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t11","@type":"Dataset","description":"Measured correlation function for the $\\Lambda\\mathrm{K^{-}}\\oplus\\overline{\\Lambda}\\mathrm{K^{+}}$ system in the 10--30\\% centrality interval.","name":"Figure 2e ALICE"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t12","@type":"Dataset","description":"THERMINATOR 2 simulation correlation function for the $\\Lambda\\mathrm{K^{-}}\\oplus\\overline{\\Lambda}\\mathrm{K^{+}}$ system in the 10--30\\% centrality interval.","name":"Figure 2e THERM"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t13","@type":"Dataset","description":"Measured correlation function for the $\\Lambda\\mathrm{K^{0}_{S}}\\oplus\\overline{\\Lambda}\\mathrm{K^{0}_{S}}$ system in the 10--30\\% centrality interval.","name":"Figure 2f ALICE"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t14","@type":"Dataset","description":"THERMINATOR 2 simulation correlation function for the $\\Lambda\\mathrm{K^{0}_{S}}\\oplus\\overline{\\Lambda}\\mathrm{K^{0}_{S}}$ system in the 10--30\\% centrality interval.","name":"Figure 2f THERM"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t15","@type":"Dataset","description":"Measured correlation function for the $\\Lambda\\mathrm{K^{+}}\\oplus\\overline{\\Lambda}\\mathrm{K^{-}}$ system in the 30--50\\% centrality interval.","name":"Figure 2g ALICE"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t16","@type":"Dataset","description":"THERMINATOR 2 simulation correlation function for the $\\Lambda\\mathrm{K^{+}}\\oplus\\overline{\\Lambda}\\mathrm{K^{-}}$ system in the 30--50\\% centrality interval.","name":"Figure 2g THERM"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t17","@type":"Dataset","description":"Measured correlation function for the $\\Lambda\\mathrm{K^{-}}\\oplus\\overline{\\Lambda}\\mathrm{K^{+}}$ system in the 30--50\\% centrality interval.","name":"Figure 2h ALICE"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t18","@type":"Dataset","description":"THERMINATOR 2 simulation correlation function for the $\\Lambda\\mathrm{K^{-}}\\oplus\\overline{\\Lambda}\\mathrm{K^{+}}$ system in the 30--50\\% centrality interval.","name":"Figure 2h THERM"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t19","@type":"Dataset","description":"Measured correlation function for the $\\Lambda\\mathrm{K^{0}_{S}}\\oplus\\overline{\\Lambda}\\mathrm{K^{0}_{S}}$ system in the 30--50\\% centrality interval.","name":"Figure 2i ALICE"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t20","@type":"Dataset","description":"THERMINATOR 2 simulation correlation function for the $\\Lambda\\mathrm{K^{0}_{S}}\\oplus\\overline{\\Lambda}\\mathrm{K^{0}_{S}}$ system in the 30--50\\% centrality interval.","name":"Figure 2i THERM"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t21","@type":"Dataset","description":"Measured correlation function for the $\\Lambda\\mathrm{K^{+}}\\oplus\\overline{\\Lambda}\\mathrm{K^{-}}$ system in the 0--10\\% centrality interval.","name":"Figure 3a"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t22","@type":"Dataset","description":"Measured correlation function for the $\\Lambda\\mathrm{K^{-}}\\oplus\\overline{\\Lambda}\\mathrm{K^{+}}$ system in the 0--10\\% centrality interval.","name":"Figure 3b"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t23","@type":"Dataset","description":"Measured correlation function for the $\\Lambda\\mathrm{K^{0}_{S}}\\oplus\\overline{\\Lambda}\\mathrm{K^{0}_{S}}$ system in the 0--10\\% centrality interval.","name":"Figure 3c"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t24","@type":"Dataset","description":"Measured correlation function for the $\\Lambda\\mathrm{K^{+}}\\oplus\\overline{\\Lambda}\\mathrm{K^{-}}$ system in the 10--30\\% centrality interval.","name":"Figure 3d"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t25","@type":"Dataset","description":"Measured correlation function for the $\\Lambda\\mathrm{K^{-}}\\oplus\\overline{\\Lambda}\\mathrm{K^{+}}$ system in the 10--30\\% centrality interval.","name":"Figure 3e"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t26","@type":"Dataset","description":"Measured correlation function for the $\\Lambda\\mathrm{K^{0}_{S}}\\oplus\\overline{\\Lambda}\\mathrm{K^{0}_{S}}$ system in the 10--30\\% centrality interval.","name":"Figure 3f"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t27","@type":"Dataset","description":"Measured correlation function for the $\\Lambda\\mathrm{K^{+}}\\oplus\\overline{\\Lambda}\\mathrm{K^{-}}$ system in the 30--50\\% centrality interval.","name":"Figure 3g"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t28","@type":"Dataset","description":"Measured correlation function for the $\\Lambda\\mathrm{K^{-}}\\oplus\\overline{\\Lambda}\\mathrm{K^{+}}$ system in the 30--50\\% centrality interval.","name":"Figure 3h"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t29","@type":"Dataset","description":"Measured correlation function for the $\\Lambda\\mathrm{K^{0}_{S}}\\oplus\\overline{\\Lambda}\\mathrm{K^{0}_{S}}$ system in the 30--50\\% centrality interval.","name":"Figure 3i"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t30","@type":"Dataset","description":"Extracted imaginary and real components of the complex scattering length, $\\Im f_{0}$ and $\\Re f_{0}$, for the $\\Lambda\\mathrm{K^{0}_{S}}$ system.","name":"Figure 4a left LamKs"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t31","@type":"Dataset","description":"Extracted imaginary and real components of the complex scattering length, $\\Im f_{0}$ and $\\Re f_{0}$, for the $\\Lambda\\mathrm{K^{-}}$ system.","name":"Figure 4a left LamKchM"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t32","@type":"Dataset","description":"Extracted imaginary and real components of the complex scattering length, $\\Im f_{0}$ and $\\Re f_{0}$, for the $\\Lambda\\mathrm{K^{+}}$ system.","name":"Figure 4a left LamKchP"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t33","@type":"Dataset","description":"Extracted effective range of the interaction, $d_{0}$, for the $\\Lambda\\mathrm{K^{0}_{S}}$ system.","name":"Figure 4a right LamKs"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t34","@type":"Dataset","description":"Extracted effective range of the interaction, $d_{0}$, for the $\\Lambda\\mathrm{K^{-}}$ system.","name":"Figure 4a right LamKchM"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t35","@type":"Dataset","description":"Extracted effective range of the interaction, $d_{0}$, for the $\\Lambda\\mathrm{K^{+}}$ system.","name":"Figure 4a right LamKchP"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t36","@type":"Dataset","description":"The extracted $\\lambda_{\\mathrm{Fit}}$ and radius parameter for the $\\Lambda$K system in the 0--10\\% centrality interval.","name":"Figure 4b 0010"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t37","@type":"Dataset","description":"The extracted $\\lambda_{\\mathrm{Fit}}$ and radius parameter for the $\\Lambda$K system in the 10--30\\% centrality interval.","name":"Figure 4b 1030"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t38","@type":"Dataset","description":"The extracted $\\lambda_{\\mathrm{Fit}}$ and radius parameter for the $\\Lambda$K system in the 30--50\\% centrality interval.","name":"Figure 4b 3050"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t39","@type":"Dataset","description":"Extracted fit $R_{\\mathrm{inv}}$ parameters as a function of pair transverse mass ($m_{\\mathrm{T}}$) for the $\\Lambda$K system in the 0--10\\% centrality...","name":"Figure 5 0010"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t40","@type":"Dataset","description":"Extracted fit $R_{\\mathrm{inv}}$ parameters as a function of pair transverse mass ($m_{\\mathrm{T}}$) for the $\\Lambda$K system in the 10--30\\% centrality...","name":"Figure 5 1030"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t41","@type":"Dataset","description":"Extracted fit $R_{\\mathrm{inv}}$ parameters as a function of pair transverse mass ($m_{\\mathrm{T}}$) for the $\\Lambda$K system in the 30--50\\% centrality...","name":"Figure 5 3050"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t42","@type":"Dataset","description":"Spherical harmonics component $C_{00}$ of the $\\Lambda\\mathrm{K^{+}}$ correlation function for the 0--10\\% centrality interval.","name":"Figure 6a"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t43","@type":"Dataset","description":"Spherical harmonics component $\\Re C_{11}$ of the $\\Lambda\\mathrm{K^{+}}$ correlation function for the 0--10\\% centrality interval.","name":"Figure 6b"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t44","@type":"Dataset","description":"Correlation functions for the $\\Lambda\\mathrm{K^{+}}\\oplus\\overline{\\Lambda}\\mathrm{K^{-}}$ system built using the normal mixed-event reference distribution for the 0--10\\% centrality interval.","name":"Figure 7a Normal"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t45","@type":"Dataset","description":"Correlation functions for the $\\Lambda\\mathrm{K^{+}}\\oplus\\overline{\\Lambda}\\mathrm{K^{-}}$ system built using the Stavinskiy method for the 0--10\\% centrality interval.","name":"Figure 7a Stavinskiy"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t46","@type":"Dataset","description":"Correlation functions for the $\\Lambda\\mathrm{K^{+}}\\oplus\\overline{\\Lambda}\\mathrm{K^{-}}$ system built using the normal mixed-event reference distribution for the 10--30\\% centrality interval.","name":"Figure 7b Normal"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t47","@type":"Dataset","description":"Correlation functions for the $\\Lambda\\mathrm{K^{+}}\\oplus\\overline{\\Lambda}\\mathrm{K^{-}}$ system built using the Stavinskiy method for the 10--30\\% centrality interval.","name":"Figure 7b Stavinskiy"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t48","@type":"Dataset","description":"Correlation functions for the $\\Lambda\\mathrm{K^{+}}\\oplus\\overline{\\Lambda}\\mathrm{K^{-}}$ system built using the normal mixed-event reference distribution for the 30--50\\% centrality interval.","name":"Figure 7c Normal"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t49","@type":"Dataset","description":"Correlation functions for the $\\Lambda\\mathrm{K^{+}}\\oplus\\overline{\\Lambda}\\mathrm{K^{-}}$ system built using the Stavinskiy method for the 30--50\\% centrality interval.","name":"Figure 7c Stavinskiy"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t50","@type":"Dataset","description":"One-dimensional $\\Lambda\\mathrm{K^{+}}\\oplus\\overline{\\Lambda}\\mathrm{K^{-}}$ correlation function for the experimental data in the 0--10\\% centrality interval.","name":"Figure 8a ALICE"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t51","@type":"Dataset","description":"One-dimensional $\\Lambda\\mathrm{K^{+}}\\oplus\\overline{\\Lambda}\\mathrm{K^{-}}$ correlation function for the THERMINATOR 2 simulation with impact parameter b = 2 fm.","name":"Figure 8a THERM"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t52","@type":"Dataset","description":"$\\Re C_{11}$ component of a spherical harmonic decomposition for the experimental data in the 0--10\\% centrality interval.","name":"Figure 8b ALICE"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t53","@type":"Dataset","description":"$\\Re C_{11}$ component of a spherical harmonic decomposition for the THERMINATOR 2 simulation with impact parameter b = 2 fm.","name":"Figure 8b THERM"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t54","@type":"Dataset","description":"The pair source distribution from the THERMINATOR 2 simulation in the out direction.","name":"Figure 8c"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t55","@type":"Dataset","description":"The pair source distribution from the THERMINATOR 2 simulation in the side direction.","name":"Figure 8d"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t56","@type":"Dataset","description":"The pair source distribution from the THERMINATOR 2 simulation in the long direction.","name":"Figure 8e"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t57","@type":"Dataset","description":"The temporal characteristics of the pair source distribution from the THERMINATOR 2 simulation.","name":"Figure 8f"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t58","@type":"Dataset","description":"Probing the effect of varying the source shift in the outward direction, $\\mu_{\\mathrm{out}}$, within the THERMINATOR 2 framework. To achieve...","name":"Figure 9a"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t59","@type":"Dataset","description":"Probing the effect of varying the source shift in the outward direction, $\\mu_{\\mathrm{out}}$, within the THERMINATOR 2 framework. To achieve...","name":"Figure 9b"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t60","@type":"Dataset","description":"Probing the effect of varying the source shift in the outward direction, $\\mu_{\\mathrm{out}}$, within the THERMINATOR 2 framework. To achieve...","name":"Figure 9c"},{"@id":"https://doi.org/10.17182/hepdata.104979.v1/t61","@type":"Dataset","description":"Probing the effect of varying the source shift in the outward direction, $\\mu_{\\mathrm{out}}$, within the THERMINATOR 2 framework. 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