{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.47487.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/440721"}},{"@id":"https://doi.org/10.1007/s002880050462","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"OPAL Collaboration"},"creator":{"@type":"Organization","name":"OPAL Collaboration"},"datePublished":"1997","description":"CERN-LEP. Measurement of hadron and event shape distributions in e+ e- interactions at centre-of -mass energies of 161 GeV. Fits to the data give alpha_s (161 Gev) to be 0.101 +- 0.005 (DSYS=0.007), and the position of the peak in the ln(l/x) distribution to be 4.00 +- 0.03 (DSYS=0.02).","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.47487.v1/t1","@type":"Dataset","description":"Determination of alpha_s.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.47487.v1/t2","@type":"Dataset","description":"Multiplicity and higher moments.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.47487.v1/t3","@type":"Dataset","description":"Thrust distribution.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.47487.v1/t4","@type":"Dataset","description":"Tmajor distribution.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.47487.v1/t5","@type":"Dataset","description":"Tminor distribution.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.47487.v1/t6","@type":"Dataset","description":"Oblateness distribution.","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.47487.v1/t7","@type":"Dataset","description":"Sphericity distribution.","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.47487.v1/t8","@type":"Dataset","description":"Aplanarity distribution.","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.47487.v1/t9","@type":"Dataset","description":"C-parameter distribution.","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.47487.v1/t10","@type":"Dataset","description":"Heavy Jet Mass distribution.","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.47487.v1/t11","@type":"Dataset","description":"Total Jet Broadening distribution.","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.47487.v1/t12","@type":"Dataset","description":"Wide Jet Broadening distribution.","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.47487.v1/t13","@type":"Dataset","description":"The mean of the event shape distributions.","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.47487.v1/t14","@type":"Dataset","description":"The width of the event shape distributions.","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.47487.v1/t15","@type":"Dataset","description":"The skewness of the event shape distributions.","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.47487.v1/t16","@type":"Dataset","description":"Jet rates using the JADE E0 scheme as a function of ycut (the cut-off parameter).","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.47487.v1/t17","@type":"Dataset","description":"Jet rates using the Durham Scheme as a function of ycut (the cut-off parameter).","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.47487.v1/t18","@type":"Dataset","description":"Jet rates using the Cone algorithm as a function of the cone size R. Minimum jet energy is fixed at...","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.47487.v1/t19","@type":"Dataset","description":"Jet rates using the Cone algorithm as a function of the minimum jet energy. The cone size is fixed at...","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.47487.v1/t20","@type":"Dataset","description":"Differential two jet rate using the Durham jet finding algorithm.","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.47487.v1/t21","@type":"Dataset","description":"PTIN distribution.","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.47487.v1/t22","@type":"Dataset","description":"PTOUT distribution.","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.47487.v1/t23","@type":"Dataset","description":"Rapidity distribution of charged particles.","name":"Table 23"},{"@id":"https://doi.org/10.17182/hepdata.47487.v1/t24","@type":"Dataset","description":"Fragmentation function.","name":"Table 24"},{"@id":"https://doi.org/10.17182/hepdata.47487.v1/t25","@type":"Dataset","description":"The ln(1/xe) distribution.","name":"Table 25"},{"@id":"https://doi.org/10.17182/hepdata.47487.v1/t26","@type":"Dataset","description":"Multiplicity distribution of charged particles.","name":"Table 26"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins440721?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/47487"}],"inLanguage":"en","name":"QCD studies with e+ e- annihilation data at 161-GeV.","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins440721?version=1","version":1}