{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.12882.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/513337"}},{"@id":"https://doi.org/10.1007/s100520000432","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":[{"@type":"Organization","name":"JADE Collaboration"},{"@type":"Organization","name":"OPAL Collaboration"}],"creator":[{"@type":"Organization","name":"JADE Collaboration"},{"@type":"Organization","name":"OPAL Collaboration"}],"datePublished":"2000","description":"CERN and DESY. Measurments of jet-multiplicity related observables in E+E- annihilations in the c.m. energy range from 35 to 189 GeV using data taken by the JADE and OPAL experiments. The observables are obtained using the JADE, Durham, Cambridge and cone finding jet alogrithms. The observables measured are the N-jet rates, the mean jet multiplicities, the differential cross sections w.r.t. Yn,n+1 and the differential N-jet fractions. The strong coupling constant ALPHAS is determined at each energy by fits to O(alpha_s**2) calculations, as well as matched O(alpha_s**2) and NLLA predictions to the data.. This is PART 1 of the record and gives the ALPHAS results. PART 2 gives the measured observables using the JADE jet finding alogrithm. PART 3 gives the measured observables using the DURHAM jet finding alogrithm. PART 4 gives the measured observables using the CAMBRIDGE jet finding alogrithm. PART 5 gives the measured observables using the CONE jet finding alogrithm. Numerical values supplied by P Pfeifenschneider.\nCERN and DESY. Measurments of jet-multiplicity related observables in E+E- annihilations in the c.m. energy range from 35 to 189 GeV using data taken by the JADE and OPAL experiments. The observables are obtained using the JADE, Durham, Cambridge and cone finding jet alogrithms. The observables measured are the N-jet rates, the mean jet multiplicities, the differential cross sections w.r.t. Yn,n+1 and the differential N-jet fractions. The strong coupling constant ALPHAS is determined at each energy by fits to O(alpha_s**2) calculations, as well as matched O(alpha_s**2) and NLLA predictions to the data.. PART 1 of the record gives the ALPHAS results. This is PART 2 and gives the measured observables using the JADE jet finding alogrithm. PART 3 gives the measured observables using the DURHAM jet finding alogrithm. PART 4 gives the measured observables using the CAMBRIDGE jet finding alogrithm. PART 5 gives the measured observables using the CONE jet finding alogrithm. Numerical values supplied by P Pfeifenschneider.\nCERN and DESY. Measurments of jet-multiplicity related observables in E+E- annihilations in the c.m. energy range from 35 to 189 GeV using data taken by the JADE and OPAL experiments. The observables are obtained using the JADE, Durham, Cambridge and cone finding jet alogrithms. The observables measured are the N-jet rates, the mean jet multiplicities, the differential cross sections w.r.t. Yn,n+1 and the differential N-jet fractions. The strong coupling constant ALPHAS is determined at each energy by fits to O(alpha_s**2) calculations, as well as matched O(alpha_s**2) and NLLA predictions to the data.. PART 1 of the record gives the ALPHAS results. PART 2 gives the measured observables using the JADE jet finding alogrithm. This is PART 3 and gives the measured observables using the DURHAM jet finding alogrithm. PART 4 gives the measured observables using the CAMBRIDGE jet finding alogrithm. PART 5 gives the measured observables using the CONE jet finding alogrithm. Numerical values supplied by P Pfeifenschneider.\nCERN and DESY. Measurments of jet-multiplicity related observables in E+E- annihilations in the c.m. energy range from 35 to 189 GeV using data taken by the JADE and OPAL experiments. The observables are obtained using the JADE, Durham, Cambridge and cone finding jet alogrithms. The observables measured are the N-jet rates, the mean jet multiplicities, the differential cross sections w.r.t. Yn,n+1 and the differential N-jet fractions. The strong coupling constant ALPHAS is determined at each energy by fits to O(alpha_s**2) calculations, as well as matched O(alpha_s**2) and NLLA predictions to the data.. PART 1 of the record gives the ALPHAS results. PART 2 gives the measured observables using the JADE jet finding alogrithm. PART 3 gives the measured observables using the DURHAM jet finding alogrithm. This is PART 4 and gives the measured observables using the CAMBRIDGE jet finding alogrithm. PART 5 gives the measured observables using the CONE jet finding alogrithm. Numerical values supplied by P Pfeifenschneider.\nCERN and DESY. Measurments of jet-multiplicity related observables in E+E- annihilations in the c.m. energy range from 35 to 189 GeV using data taken by the JADE and OPAL experiments. The observables are obtained using the JADE, Durham, Cambridge and cone finding jet alogrithms. The observables measured are the N-jet rates, the mean jet multiplicities, the differential cross sections w.r.t. Yn,n+1 and the differential N-jet fractions. The strong coupling constant ALPHAS is determined at each energy by fits to O(alpha_s**2) calculations, as well as matched O(alpha_s**2) and NLLA predictions to the data.. PART 1 of the record gives the ALPHAS results. PART 2 gives the measured observables using the JADE jet finding alogrithm. PART 3 gives the measured observables using the DURHAM jet finding alogrithm. PART 4 gives the measured observables using the CAMBRIDGE jet fin...","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t1","@type":"Dataset","description":"Overall result for ALPHAS at the Z0 mass from the combination of the ln R-matching results from the observables evolved...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t2","@type":"Dataset","description":"Weighted mean for ALPHAS at the Z0 mass determined from the energy evolutions of the mean values of the 2-jet...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t3","@type":"Dataset","description":"Combined results for ALPHA_S from fits of matched predicitions. The first systematic (DSYS) error is the experimental systematic, the second...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t4","@type":"Dataset","description":"Results for ALPHAS from fits of the ln R-matching predictions for the fractional 2-jet rate observable (D2), and the mean...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t5","@type":"Dataset","description":"Results for ALPHAS at the Z0 mass from fits of the O(alphas**2) predicitonsfor the energy evolution of the mean 2-jet...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t6","@type":"Dataset","description":"Results for ALPHAS at the Z0 mass from fits of the O(alphas**2) predicitonsfor the 3-jet fractions (R3) for the JADE,...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t7","@type":"Dataset","description":"N-Jet rates from the JADE collaboration at c.m. energy 35 GeV. Jets define using the JADE/E0 alogrithm.","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t8","@type":"Dataset","description":"N-Jet rates from the JADE collaboration at c.m. energy 44 GeV. Jets define using the JADE/E0 alogrithm.","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t9","@type":"Dataset","description":"N-Jet rates from the OPAL collaboration at c.m. energy 91 GeV. Jets define using the JADE/E0 alogrithm.","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t10","@type":"Dataset","description":"N-Jet rates from the OPAL collaboration at c.m. energy 133 GeV. Jets define using the JADE/E0 alogrithm.","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t11","@type":"Dataset","description":"N-Jet rates from the OPAL collaboration at c.m. energy 161 GeV. Jets define using the JADE/E0 alogrithm.","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t12","@type":"Dataset","description":"N-Jet rates from the OPAL collaboration at c.m. energy 172 GeV. Jets define using the JADE/E0 alogrithm.","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t13","@type":"Dataset","description":"N-Jet rates from the OPAL collaboration at c.m. energy 183 GeV. Jets define using the JADE/E0 alogrithm.","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t14","@type":"Dataset","description":"N-Jet rates from the OPAL collaboration at c.m. energy 189 GeV. Jets define using the JADE/E0 alogrithm.","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t15","@type":"Dataset","description":"Mean value of the observable Ynm (the value of YCUT at the boundary betweenn and (n+1=m) jets) as a function...","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t16","@type":"Dataset","description":"N-Jet rates from the JADE collaboration at c.m. energy 35 GeV. Jets defined using the DURHAM alogrithm.","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t17","@type":"Dataset","description":"N-Jet rates from the JADE collaboration at c.m. energy 44 GeV. Jets defined using the DURHAM alogrithm.","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t18","@type":"Dataset","description":"N-Jet rates from the OPAL collaboration at c.m. energy 91 GeV. Jets defined using the DURHAM alogrithm.","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t19","@type":"Dataset","description":"N-Jet rates from the OPAL collaboration at c.m. energy 133 GeV. Jets defined using the DURHAM alogrithm.","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t20","@type":"Dataset","description":"N-Jet rates from the OPAL collaboration at c.m. energy 161 GeV. Jets defined using the DURHAM alogrithm.","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t21","@type":"Dataset","description":"N-Jet rates from the OPAL collaboration at c.m. energy 172 GeV. Jets defined using the DURHAM alogrithm.","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t22","@type":"Dataset","description":"N-Jet rates from the OPAL collaboration at c.m. energy 183 GeV. Jets defined using the DURHAM alogrithm.","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t23","@type":"Dataset","description":"N-Jet rates from the OPAL collaboration at c.m. energy 189 GeV. Jets defined using the DURHAM alogrithm.","name":"Table 23"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t24","@type":"Dataset","description":"Differential distributions in Ynm (the minimum YCUT for the separation inton and m(=n+1) jets). ) from the JADE collaboration at...","name":"Table 24"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t25","@type":"Dataset","description":"Differential distributions in Ynm (the minimum YCUT for the separation inton and m(=n+1) jets). ) from the JADE collaboration at...","name":"Table 25"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t26","@type":"Dataset","description":"Differential distributions in Ynm (the minimum YCUT for the separation inton and m(=n+1) jets). ) from the OPAL collaboration at...","name":"Table 26"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t27","@type":"Dataset","description":"Differential distributions in Ynm (the minimum YCUT for the separation inton and m(=n+1) jets). ) from the OPAL collaboration at...","name":"Table 27"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t28","@type":"Dataset","description":"Differential distributions in Ynm (the minimum YCUT for the separation inton and m(=n+1) jets). ) from the OPAL collaboration at...","name":"Table 28"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t29","@type":"Dataset","description":"Differential distributions in Ynm (the minimum YCUT for the separation inton and m(=n+1) jets). ) from the OPAL collaboration at...","name":"Table 29"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t30","@type":"Dataset","description":"Differential distributions in Ynm (the minimum YCUT for the separation inton and m(=n+1) jets). ) from the OPAL collaboration at...","name":"Table 30"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t31","@type":"Dataset","description":"Differential distributions in Ynm (the minimum YCUT for the separation inton and m(=n+1) jets). ) from the OPAL collaboration at...","name":"Table 31"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t32","@type":"Dataset","description":"Mean jet multiplicity as a function of YCUT from the JADE collaboration at c.m. energy 35 GeV. Jets defined using...","name":"Table 32"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t33","@type":"Dataset","description":"Mean jet multiplicity as a function of YCUT from the JADE collaboration at c.m. energy 44 GeV. Jets defined using...","name":"Table 33"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t34","@type":"Dataset","description":"Mean jet multiplicity as a function of YCUT from the OPAL collaboration at c.m. energy 91 GeV. Jets defined using...","name":"Table 34"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t35","@type":"Dataset","description":"Mean jet multiplicity as a function of YCUT from the OPAL collaboration at c.m. energy 133 GeV. Jets defined using...","name":"Table 35"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t36","@type":"Dataset","description":"Mean jet multiplicity as a function of YCUT from the OPAL collaboration at c.m. energy 161 GeV. Jets defined using...","name":"Table 36"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t37","@type":"Dataset","description":"Mean jet multiplicity as a function of YCUT from the OPAL collaboration at c.m. energy 172 GeV. Jets defined using...","name":"Table 37"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t38","@type":"Dataset","description":"Mean jet multiplicity as a function of YCUT from the OPAL collaboration at c.m. energy 183 GeV. Jets defined using...","name":"Table 38"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t39","@type":"Dataset","description":"Mean jet multiplicity as a function of YCUT from the OPAL collaboration at c.m. energy 189 GeV. Jets defined using...","name":"Table 39"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t40","@type":"Dataset","description":"Mean value of the observable Ynm (the value of YCUT at the boundary betweenn and (n+1=m) jets) as a function...","name":"Table 40"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t41","@type":"Dataset","description":"N-Jet rates from the JADE collaboration at c.m. energy 35 GeV. Jets defined using the CAMBRIDGE alogrithm.","name":"Table 41"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t42","@type":"Dataset","description":"N-Jet rates from the JADE collaboration at c.m. energy 44 GeV. Jets defined using the CAMBRIDGE alogrithm.","name":"Table 42"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t43","@type":"Dataset","description":"N-Jet rates from the OPAL collaboration at c.m. energy 91 GeV. Jets defined using the CAMBRIDGE alogrithm.","name":"Table 43"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t44","@type":"Dataset","description":"N-Jet rates from the OPAL collaboration at c.m. energy 133 GeV. Jets defined using the CAMBRIDGE alogrithm.","name":"Table 44"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t45","@type":"Dataset","description":"N-Jet rates from the OPAL collaboration at c.m. energy 161 GeV. Jets defined using the CAMBRIDGE alogrithm.","name":"Table 45"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t46","@type":"Dataset","description":"N-Jet rates from the OPAL collaboration at c.m. energy 172 GeV. Jets defined using the CAMBRIDGE alogrithm.","name":"Table 46"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t47","@type":"Dataset","description":"N-Jet rates from the OPAL collaboration at c.m. energy 183 GeV. Jets defined using the CAMBRIDGE alogrithm.","name":"Table 47"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t48","@type":"Dataset","description":"N-Jet rates from the OPAL collaboration at c.m. energy 189 GeV. Jets defined using the CAMBRIDGE alogrithm.","name":"Table 48"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t49","@type":"Dataset","description":"Differential N-Jet rates from the JADE collaboration at c.m. energy 35 GeV. Jets defined using the CAMBRIDGE alogrithm.","name":"Table 49"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t50","@type":"Dataset","description":"Differential N-Jet rates from the JADE collaboration at c.m. energy 44 GeV. Jets defined using the CAMBRIDGE alogrithm.","name":"Table 50"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t51","@type":"Dataset","description":"Differential N-Jet rates from the OPAL collaboration at c.m. energy 91 GeV. Jets defined using the CAMBRIDGE alogrithm.","name":"Table 51"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t52","@type":"Dataset","description":"Differential N-Jet rates from the OPAL collaboration at c.m. energy 133 GeV. Jets defined using the CAMBRIDGE alogrithm.","name":"Table 52"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t53","@type":"Dataset","description":"Differential N-Jet rates from the OPAL collaboration at c.m. energy 161 GeV. Jets defined using the CAMBRIDGE alogrithm.","name":"Table 53"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t54","@type":"Dataset","description":"Differential N-Jet rates from the OPAL collaboration at c.m. energy 172 GeV. Jets defined using the CAMBRIDGE alogrithm.","name":"Table 54"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t55","@type":"Dataset","description":"Differential N-Jet rates from the OPAL collaboration at c.m. energy 183 GeV. 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Jets defined using...","name":"Table 59"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t60","@type":"Dataset","description":"Mean jet multiplicity as a function of YCUT from the OPAL collaboration at c.m. energy 133 GeV. Jets defined using...","name":"Table 60"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t61","@type":"Dataset","description":"Mean jet multiplicity as a function of YCUT from the OPAL collaboration at c.m. energy 161 GeV. Jets defined using...","name":"Table 61"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t62","@type":"Dataset","description":"Mean jet multiplicity as a function of YCUT from the OPAL collaboration at c.m. energy 172 GeV. Jets defined using...","name":"Table 62"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t63","@type":"Dataset","description":"Mean jet multiplicity as a function of YCUT from the OPAL collaboration at c.m. energy 183 GeV. Jets defined using...","name":"Table 63"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t64","@type":"Dataset","description":"Mean jet multiplicity as a function of YCUT from the OPAL collaboration at c.m. energy 189 GeV. Jets defined using...","name":"Table 64"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t65","@type":"Dataset","description":"N-Jet rates from JADE collaboration at c.m. energy 35 GeV. Jets define using the CONE alogrithm.","name":"Table 65"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t66","@type":"Dataset","description":"N-Jet rates from JADE collaboration at c.m. energy 35 GeV. Jets define using the CONE alogrithm.","name":"Table 66"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t67","@type":"Dataset","description":"N-Jet rates from JADE collaboration at c.m. energy 44 GeV. Jets define using the CONE alogrithm.","name":"Table 67"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t68","@type":"Dataset","description":"N-Jet rates from JADE collaboration at c.m. energy 44 GeV. Jets define using the CONE alogrithm.","name":"Table 68"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t69","@type":"Dataset","description":"N-Jet rates from OPAL collaboration at c.m. energy 91 GeV. Jets define using the CONE alogrithm.","name":"Table 69"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t70","@type":"Dataset","description":"N-Jet rates from OPAL collaboration at c.m. energy 91 GeV. Jets define using the CONE alogrithm.","name":"Table 70"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t71","@type":"Dataset","description":"N-Jet rates from OPAL collaboration at c.m. energy 133 GeV. Jets define using the CONE alogrithm.","name":"Table 71"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t72","@type":"Dataset","description":"N-Jet rates from OPAL collaboration at c.m. energy 133 GeV. Jets define using the CONE alogrithm.","name":"Table 72"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t73","@type":"Dataset","description":"N-Jet rates from OPAL collaboration at c.m. energy 161 GeV. Jets define using the CONE alogrithm.","name":"Table 73"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t74","@type":"Dataset","description":"N-Jet rates from OPAL collaboration at c.m. energy 161 GeV. Jets define using the CONE alogrithm.","name":"Table 74"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t75","@type":"Dataset","description":"N-Jet rates from OPAL collaboration at c.m. energy 172 GeV. Jets define using the CONE alogrithm.","name":"Table 75"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t76","@type":"Dataset","description":"N-Jet rates from OPAL collaboration at c.m. energy 172 GeV. Jets define using the CONE alogrithm.","name":"Table 76"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t77","@type":"Dataset","description":"N-Jet rates from OPAL collaboration at c.m. energy 183 GeV. Jets define using the CONE alogrithm.","name":"Table 77"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t78","@type":"Dataset","description":"N-Jet rates from OPAL collaboration at c.m. energy 183 GeV. Jets define using the CONE alogrithm.","name":"Table 78"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t79","@type":"Dataset","description":"N-Jet rates from OPAL collaboration at c.m. energy 189 GeV. Jets define using the CONE alogrithm.","name":"Table 79"},{"@id":"https://doi.org/10.17182/hepdata.12882.v1/t80","@type":"Dataset","description":"N-Jet rates from OPAL collaboration at c.m. energy 189 GeV. Jets define using the CONE alogrithm.","name":"Table 80"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins513337?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/12882"}],"inLanguage":"en","name":"QCD analyses and determinations of alpha(s) in e+ e- annihilation at energies between 35-GeV and 189-GeV.","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins513337?version=1","version":1}