{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.155473.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2791620"}},{"@id":"https://doi.org/10.1103/PhysRevC.110.064901","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2024","description":"Transverse momentum spectra of deuterons and 3He nuclei, measured in Xe--Xe collisions at centre-of-mass per nucleon-nucleon energy of 5.44 TeV, are shown in Fig. 3. The coalescence parameters B2 and B3 as a function of the transverse momentum per nucleon are reported in Fig. 7. The ratios of the integrated yields of deuterons to protons and 3He to protons are shown in Fig. 5 as a function of the average charged particle multiplicity density. The ratios of the integrated yields of deuterons to pions and 3He to pions are shown in Fig. 6 as a function of the average charged particle multiplicity density. The coalescence parameter B2 as a function of the average charged particle multiplicity density is not shown in the paper but the data are reported in Table 17. Finally, in Fig. 8 the elliptic flow v2 is shown.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.155473.v1/t1","@type":"Dataset","description":"Transverse momentum spectra of 3He nuclei measured in Xe--Xe collisions at centre-of-mass per nucleon-nucleon energy of 5.44 TeV, as shown...","name":"Table 1 - 3He PT spectrum "},{"@id":"https://doi.org/10.17182/hepdata.155473.v1/t2","@type":"Dataset","description":"Transverse momentum spectra of deuterons measured in Xe--Xe collisions at centre-of-mass per nucleon-nucleon energy of 5.44 TeV, as shown in...","name":"Table 2 - Deuteron PT spectrum centrality 0 to 10"},{"@id":"https://doi.org/10.17182/hepdata.155473.v1/t3","@type":"Dataset","description":"Transverse momentum spectra of deuterons measured in Xe--Xe collisions at centre-of-mass per nucleon-nucleon energy of 5.44 TeV, as shown in...","name":"Table 3 - Deuteron PT spectrum centrality 10 to 20"},{"@id":"https://doi.org/10.17182/hepdata.155473.v1/t4","@type":"Dataset","description":"Transverse momentum spectra of deuterons measured in Xe--Xe collisions at centre-of-mass per nucleon-nucleon energy of 5.44 TeV, as shown in...","name":"Table 4 - Deuteron PT spectrum centrality 20 to 40"},{"@id":"https://doi.org/10.17182/hepdata.155473.v1/t5","@type":"Dataset","description":"Transverse momentum spectra of deuterons measured in Xe--Xe collisions at centre-of-mass per nucleon-nucleon energy of 5.44 TeV, as shown in...","name":"Table 5 - Deuteron PT spectrum centrality 40 to 60"},{"@id":"https://doi.org/10.17182/hepdata.155473.v1/t6","@type":"Dataset","description":"Transverse momentum spectra of deuterons measured in Xe--Xe collisions at centre-of-mass per nucleon-nucleon energy of 5.44 TeV, as shown in...","name":"Table 6 - Deuteron PT spectrum centrality 60 to 90"},{"@id":"https://doi.org/10.17182/hepdata.155473.v1/t7","@type":"Dataset","description":"Coalescence parameter B2 as a function of the transverse momentum per nucleon pT/A, in the centrality class 0 to 10...","name":"Table 7 - B2 vs PTA centrality 0 to 10"},{"@id":"https://doi.org/10.17182/hepdata.155473.v1/t8","@type":"Dataset","description":"Coalescence parameter B2 as a function of the transverse momentum per nucleon pT/A, in the centrality class 10 to 20...","name":"Table 8 - B2 vs PTA centrality 10 to 20"},{"@id":"https://doi.org/10.17182/hepdata.155473.v1/t9","@type":"Dataset","description":"Coalescence parameter B2 as a function of the transverse momentum per nucleon pT/A, in the centrality class 20 to 40...","name":"Table 9 - B2 vs PTA centrality 20 to 40"},{"@id":"https://doi.org/10.17182/hepdata.155473.v1/t10","@type":"Dataset","description":"Coalescence parameter B2 as a function of the transverse momentum per nucleon pT/A, in the centrality class 40 to 60...","name":"Table 10 - B2 vs PTA centrality 40 to 60"},{"@id":"https://doi.org/10.17182/hepdata.155473.v1/t11","@type":"Dataset","description":"Coalescence parameter B2 as a function of the transverse momentum per nucleon pT/A, in the centrality class 60 to 90...","name":"Table 11 - B2 vs PTA centrality 60 to 90"},{"@id":"https://doi.org/10.17182/hepdata.155473.v1/t12","@type":"Dataset","description":"Coalescence parameter B3 as a function of the transverse momentum per nucleon pT/A, in the centrality class 0 to 90...","name":"Table 12 - B3 vs PTA centrality 0 to 90"},{"@id":"https://doi.org/10.17182/hepdata.155473.v1/t13","@type":"Dataset","description":"Ratio of integrated yields of deuterons and of protons, as a function of the average charged particle multiplicity density. The...","name":"Table 13 - Deuteron-over-proton yields vs multiplicity"},{"@id":"https://doi.org/10.17182/hepdata.155473.v1/t14","@type":"Dataset","description":"Ratio of integrated yields of He3 and of protons, as a function of the average charged particle multiplicity density. The...","name":"Table 14 - He3-over-proton yields vs multiplicity"},{"@id":"https://doi.org/10.17182/hepdata.155473.v1/t15","@type":"Dataset","description":"Ratio of integrated yields of deuterons and of pions, as a function of the average charged particle multiplicity density. The...","name":"Table 15 - Deuteron-over-pion yields vs multiplicity"},{"@id":"https://doi.org/10.17182/hepdata.155473.v1/t16","@type":"Dataset","description":"Ratio of integrated yields of He3 and of pions, as a function of the average charged particle multiplicity density. The...","name":"Table 16 - He3-over-pion yields vs multiplicity"},{"@id":"https://doi.org/10.17182/hepdata.155473.v1/t17","@type":"Dataset","description":"B2 as a function of the average charged particle multiplicity density for pT-over-A equal to 0.75 GEV. The B2 vs....","name":"Table 17 - B2 vs multiplicity"},{"@id":"https://doi.org/10.17182/hepdata.155473.v1/t18","@type":"Dataset","description":"(Anti)deuteron $v_2$ measured at midrapidity in the 0-20 centrality class, as shown in Fig. 8 (left panel).","name":"Table 18 -  v2 (elliptic flow) deuterons 0-20"},{"@id":"https://doi.org/10.17182/hepdata.155473.v1/t19","@type":"Dataset","description":"(Anti)deuteron $v_2$ measured at midrapidity in the 20-40 centrality class, as shown in Fig. 8 (right panel).","name":"Table 19 -  v2 (elliptic flow) deuterons 20-40"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2791620?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/155473"}],"inLanguage":"en","name":"Measurement of the production and elliptic flow of (anti)nuclei in Xe-Xe collisions at $\\sqrt{s_{\\rm NN}}$ = 5.44 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins2791620?version=1","version":1}