{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.129149.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1891385"}},{"@id":"https://doi.org/10.1007/JHEP05(2022)061","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2022","description":"The jet angularities are a class of jet substructure observables which characterize the angular and momentum distribution of particles within jets. These observables are sensitive to momentum scales ranging from perturbative hard scatterings to nonperturbative fragmentation into final-state hadrons. We report measurements of several groomed and ungroomed jet angularities in pp collisions at $\\sqrt{s}=5.02$ TeV with the ALICE detector. Jets are reconstructed using charged particle tracks at midrapidity ($|\\eta| < 0.9$). The anti-$k_{\\rm T}$ algorithm is used with jet resolution parameters $R=0.2$ and $R=0.4$ for several transverse momentum $p_{\\rm T}^{\\text{ch jet}}$ intervals in the 20$-$100 GeV/$c$ range. Using the jet grooming algorithm Soft Drop, the sensitivity to softer, wide-angle processes, as well as the underlying event, can be reduced in a way which is well-controlled in theoretical calculations. We report the ungroomed jet angularities, $\\lambda_{\\alpha}$, and groomed jet angularities, $\\lambda_{\\alpha\\text{,g}}$, to investigate the interplay between perturbative and nonperturbative effects at low jet momenta. Various angular exponent parameters $\\alpha = 1$, 1.5, 2, and 3 are used to systematically vary the sensitivity of the observable to collinear and soft radiation. Results are compared to analytical predictions at next-to-leading-logarithmic accuracy, which provide a generally good description of the data in the perturbative regime but exhibit discrepancies in the nonperturbative regime. Moreover, these measurements serve as a baseline for future ones in heavy-ion collisions by providing new insight into the interplay between perturbative and nonperturbative effects in the angular and momentum substructure of jets. They supply crucial guidance on the selection of jet resolution parameter, jet transverse momentum, and angular scaling variable for jet quenching studies.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t1","@type":"Dataset","description":"Jet angularity $\\lambda_{\\alpha}$ for $\\alpha = 1$. $20&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;40$. For the \"trkeff\" and \"generator\" systematic uncertainty sources, the signed systematic...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t2","@type":"Dataset","description":"Jet angularity $\\lambda_{\\alpha}$ for $\\alpha = 1.5$. $20&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;40$. For the \"trkeff\" and \"generator\" systematic uncertainty sources, the signed systematic...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t3","@type":"Dataset","description":"Jet angularity $\\lambda_{\\alpha}$ for $\\alpha = 2$. $20&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;40$. For the \"trkeff\" and \"generator\" systematic uncertainty sources, the signed systematic...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t4","@type":"Dataset","description":"Jet angularity $\\lambda_{\\alpha}$ for $\\alpha = 3$. $20&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;40$. For the \"trkeff\" and \"generator\" systematic uncertainty sources, the signed systematic...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t5","@type":"Dataset","description":"Groomed jet angularity $\\lambda_{\\alpha,g}$ for $\\alpha = 1$. $20&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;40$, Soft Drop $z_{\\mathrm{cut}}=0.2, \\beta=0$. Note: The first bin corresponds to...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t6","@type":"Dataset","description":"Groomed jet angularity $\\lambda_{\\alpha,g}$ for $\\alpha = 1.5$. $20&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;40$, Soft Drop $z_{\\mathrm{cut}}=0.2, \\beta=0$. Note: The first bin corresponds to...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t7","@type":"Dataset","description":"Groomed jet angularity $\\lambda_{\\alpha,g}$ for $\\alpha = 2$. $20&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;40$, Soft Drop $z_{\\mathrm{cut}}=0.2, \\beta=0$. Note: The first bin corresponds to...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t8","@type":"Dataset","description":"Groomed jet angularity $\\lambda_{\\alpha,g}$ for $\\alpha = 3$. $20&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;40$, Soft Drop $z_{\\mathrm{cut}}=0.2, \\beta=0$. Note: The first bin corresponds to...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t9","@type":"Dataset","description":"Jet angularity $\\lambda_{\\alpha}$ for $\\alpha = 1$. $40&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;60$. For the \"trkeff\" and \"generator\" systematic uncertainty sources, the signed systematic...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t10","@type":"Dataset","description":"Jet angularity $\\lambda_{\\alpha}$ for $\\alpha = 1.5$. $40&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;60$. For the \"trkeff\" and \"generator\" systematic uncertainty sources, the signed systematic...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t11","@type":"Dataset","description":"Jet angularity $\\lambda_{\\alpha}$ for $\\alpha = 2$. $40&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;60$. For the \"trkeff\" and \"generator\" systematic uncertainty sources, the signed systematic...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t12","@type":"Dataset","description":"Jet angularity $\\lambda_{\\alpha}$ for $\\alpha = 3$. $40&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;60$. For the \"trkeff\" and \"generator\" systematic uncertainty sources, the signed systematic...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t13","@type":"Dataset","description":"Groomed jet angularity $\\lambda_{\\alpha,g}$ for $\\alpha = 1$. $40&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;60$, Soft Drop $z_{\\mathrm{cut}}=0.2, \\beta=0$. Note: The first bin corresponds to...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t14","@type":"Dataset","description":"Groomed jet angularity $\\lambda_{\\alpha,g}$ for $\\alpha = 1.5$. $40&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;60$, Soft Drop $z_{\\mathrm{cut}}=0.2, \\beta=0$. Note: The first bin corresponds to...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t15","@type":"Dataset","description":"Groomed jet angularity $\\lambda_{\\alpha,g}$ for $\\alpha = 2$. $40&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;60$, Soft Drop $z_{\\mathrm{cut}}=0.2, \\beta=0$. Note: The first bin corresponds to...","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t16","@type":"Dataset","description":"Groomed jet angularity $\\lambda_{\\alpha,g}$ for $\\alpha = 3$. $40&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;60$, Soft Drop $z_{\\mathrm{cut}}=0.2, \\beta=0$. Note: The first bin corresponds to...","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t17","@type":"Dataset","description":"Jet angularity $\\lambda_{\\alpha}$ for $\\alpha = 1$. $60&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;80$. For the \"trkeff\" and \"generator\" systematic uncertainty sources, the signed systematic...","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t18","@type":"Dataset","description":"Jet angularity $\\lambda_{\\alpha}$ for $\\alpha = 1.5$. $60&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;80$. For the \"trkeff\" and \"generator\" systematic uncertainty sources, the signed systematic...","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t19","@type":"Dataset","description":"Jet angularity $\\lambda_{\\alpha}$ for $\\alpha = 2$. $60&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;80$. For the \"trkeff\" and \"generator\" systematic uncertainty sources, the signed systematic...","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t20","@type":"Dataset","description":"Jet angularity $\\lambda_{\\alpha}$ for $\\alpha = 3$. $60&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;80$. For the \"trkeff\" and \"generator\" systematic uncertainty sources, the signed systematic...","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t21","@type":"Dataset","description":"Groomed jet angularity $\\lambda_{\\alpha,g}$ for $\\alpha = 1$. $60&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;80$, Soft Drop $z_{\\mathrm{cut}}=0.2, \\beta=0$. Note: The first bin corresponds to...","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t22","@type":"Dataset","description":"Groomed jet angularity $\\lambda_{\\alpha,g}$ for $\\alpha = 1.5$. $60&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;80$, Soft Drop $z_{\\mathrm{cut}}=0.2, \\beta=0$. Note: The first bin corresponds to...","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t23","@type":"Dataset","description":"Groomed jet angularity $\\lambda_{\\alpha,g}$ for $\\alpha = 2$. $60&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;80$, Soft Drop $z_{\\mathrm{cut}}=0.2, \\beta=0$. Note: The first bin corresponds to...","name":"Table 23"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t24","@type":"Dataset","description":"Groomed jet angularity $\\lambda_{\\alpha,g}$ for $\\alpha = 3$. $60&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;80$, Soft Drop $z_{\\mathrm{cut}}=0.2, \\beta=0$. Note: The first bin corresponds to...","name":"Table 24"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t25","@type":"Dataset","description":"Jet angularity $\\lambda_{\\alpha}$ for $\\alpha = 1$. $80&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;100$. For the \"trkeff\" and \"generator\" systematic uncertainty sources, the signed systematic...","name":"Table 25"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t26","@type":"Dataset","description":"Jet angularity $\\lambda_{\\alpha}$ for $\\alpha = 1.5$. $80&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;100$. For the \"trkeff\" and \"generator\" systematic uncertainty sources, the signed systematic...","name":"Table 26"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t27","@type":"Dataset","description":"Jet angularity $\\lambda_{\\alpha}$ for $\\alpha = 2$. $80&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;100$. For the \"trkeff\" and \"generator\" systematic uncertainty sources, the signed systematic...","name":"Table 27"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t28","@type":"Dataset","description":"Jet angularity $\\lambda_{\\alpha}$ for $\\alpha = 3$. $80&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;100$. For the \"trkeff\" and \"generator\" systematic uncertainty sources, the signed systematic...","name":"Table 28"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t29","@type":"Dataset","description":"Groomed jet angularity $\\lambda_{\\alpha,g}$ for $\\alpha = 1$. $80&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;100$, Soft Drop $z_{\\mathrm{cut}}=0.2, \\beta=0$. Note: The first bin corresponds to...","name":"Table 29"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t30","@type":"Dataset","description":"Groomed jet angularity $\\lambda_{\\alpha,g}$ for $\\alpha = 1.5$. $80&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;100$, Soft Drop $z_{\\mathrm{cut}}=0.2, \\beta=0$. Note: The first bin corresponds to...","name":"Table 30"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t31","@type":"Dataset","description":"Groomed jet angularity $\\lambda_{\\alpha,g}$ for $\\alpha = 2$. $80&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;100$, Soft Drop $z_{\\mathrm{cut}}=0.2, \\beta=0$. Note: The first bin corresponds to...","name":"Table 31"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t32","@type":"Dataset","description":"Groomed jet angularity $\\lambda_{\\alpha,g}$ for $\\alpha = 3$. $80&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;100$, Soft Drop $z_{\\mathrm{cut}}=0.2, \\beta=0$. Note: The first bin corresponds to...","name":"Table 32"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t33","@type":"Dataset","description":"Jet angularity $\\lambda_{\\alpha}$ for $\\alpha = 1$. $20&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;40$. For the \"trkeff\" and \"generator\" systematic uncertainty sources, the signed systematic...","name":"Table 33"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t34","@type":"Dataset","description":"Jet angularity $\\lambda_{\\alpha}$ for $\\alpha = 1.5$. $20&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;40$. For the \"trkeff\" and \"generator\" systematic uncertainty sources, the signed systematic...","name":"Table 34"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t35","@type":"Dataset","description":"Jet angularity $\\lambda_{\\alpha}$ for $\\alpha = 2$. $20&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;40$. For the \"trkeff\" and \"generator\" systematic uncertainty sources, the signed systematic...","name":"Table 35"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t36","@type":"Dataset","description":"Jet angularity $\\lambda_{\\alpha}$ for $\\alpha = 3$. $20&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;40$. For the \"trkeff\" and \"generator\" systematic uncertainty sources, the signed systematic...","name":"Table 36"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t37","@type":"Dataset","description":"Groomed jet angularity $\\lambda_{\\alpha,g}$ for $\\alpha = 1$. $20&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;40$, Soft Drop $z_{\\mathrm{cut}}=0.2, \\beta=0$. Note: The first bin corresponds to...","name":"Table 37"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t38","@type":"Dataset","description":"Groomed jet angularity $\\lambda_{\\alpha,g}$ for $\\alpha = 1.5$. $20&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;40$, Soft Drop $z_{\\mathrm{cut}}=0.2, \\beta=0$. Note: The first bin corresponds to...","name":"Table 38"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t39","@type":"Dataset","description":"Groomed jet angularity $\\lambda_{\\alpha,g}$ for $\\alpha = 2$. $20&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;40$, Soft Drop $z_{\\mathrm{cut}}=0.2, \\beta=0$. Note: The first bin corresponds to...","name":"Table 39"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t40","@type":"Dataset","description":"Groomed jet angularity $\\lambda_{\\alpha,g}$ for $\\alpha = 3$. $20&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;40$, Soft Drop $z_{\\mathrm{cut}}=0.2, \\beta=0$. Note: The first bin corresponds to...","name":"Table 40"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t41","@type":"Dataset","description":"Jet angularity $\\lambda_{\\alpha}$ for $\\alpha = 1$. $40&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;60$. For the \"trkeff\" and \"generator\" systematic uncertainty sources, the signed systematic...","name":"Table 41"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t42","@type":"Dataset","description":"Jet angularity $\\lambda_{\\alpha}$ for $\\alpha = 1.5$. $40&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;60$. For the \"trkeff\" and \"generator\" systematic uncertainty sources, the signed systematic...","name":"Table 42"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t43","@type":"Dataset","description":"Jet angularity $\\lambda_{\\alpha}$ for $\\alpha = 2$. $40&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;60$. For the \"trkeff\" and \"generator\" systematic uncertainty sources, the signed systematic...","name":"Table 43"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t44","@type":"Dataset","description":"Jet angularity $\\lambda_{\\alpha}$ for $\\alpha = 3$. $40&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;60$. For the \"trkeff\" and \"generator\" systematic uncertainty sources, the signed systematic...","name":"Table 44"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t45","@type":"Dataset","description":"Groomed jet angularity $\\lambda_{\\alpha,g}$ for $\\alpha = 1$. $40&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;60$, Soft Drop $z_{\\mathrm{cut}}=0.2, \\beta=0$. Note: The first bin corresponds to...","name":"Table 45"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t46","@type":"Dataset","description":"Groomed jet angularity $\\lambda_{\\alpha,g}$ for $\\alpha = 1.5$. $40&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;60$, Soft Drop $z_{\\mathrm{cut}}=0.2, \\beta=0$. Note: The first bin corresponds to...","name":"Table 46"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t47","@type":"Dataset","description":"Groomed jet angularity $\\lambda_{\\alpha,g}$ for $\\alpha = 2$. $40&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;60$, Soft Drop $z_{\\mathrm{cut}}=0.2, \\beta=0$. Note: The first bin corresponds to...","name":"Table 47"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t48","@type":"Dataset","description":"Groomed jet angularity $\\lambda_{\\alpha,g}$ for $\\alpha = 3$. $40&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;60$, Soft Drop $z_{\\mathrm{cut}}=0.2, \\beta=0$. Note: The first bin corresponds to...","name":"Table 48"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t49","@type":"Dataset","description":"Jet angularity $\\lambda_{\\alpha}$ for $\\alpha = 1$. $60&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;80$. For the \"trkeff\" and \"generator\" systematic uncertainty sources, the signed systematic...","name":"Table 49"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t50","@type":"Dataset","description":"Jet angularity $\\lambda_{\\alpha}$ for $\\alpha = 1.5$. $60&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;80$. For the \"trkeff\" and \"generator\" systematic uncertainty sources, the signed systematic...","name":"Table 50"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t51","@type":"Dataset","description":"Jet angularity $\\lambda_{\\alpha}$ for $\\alpha = 2$. $60&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;80$. For the \"trkeff\" and \"generator\" systematic uncertainty sources, the signed systematic...","name":"Table 51"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t52","@type":"Dataset","description":"Jet angularity $\\lambda_{\\alpha}$ for $\\alpha = 3$. $60&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;80$. For the \"trkeff\" and \"generator\" systematic uncertainty sources, the signed systematic...","name":"Table 52"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t53","@type":"Dataset","description":"Groomed jet angularity $\\lambda_{\\alpha,g}$ for $\\alpha = 1$. $60&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;80$, Soft Drop $z_{\\mathrm{cut}}=0.2, \\beta=0$. Note: The first bin corresponds to...","name":"Table 53"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t54","@type":"Dataset","description":"Groomed jet angularity $\\lambda_{\\alpha,g}$ for $\\alpha = 1.5$. $60&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;80$, Soft Drop $z_{\\mathrm{cut}}=0.2, \\beta=0$. Note: The first bin corresponds to...","name":"Table 54"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t55","@type":"Dataset","description":"Groomed jet angularity $\\lambda_{\\alpha,g}$ for $\\alpha = 2$. $60&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;80$, Soft Drop $z_{\\mathrm{cut}}=0.2, \\beta=0$. Note: The first bin corresponds to...","name":"Table 55"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t56","@type":"Dataset","description":"Groomed jet angularity $\\lambda_{\\alpha,g}$ for $\\alpha = 3$. $60&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;80$, Soft Drop $z_{\\mathrm{cut}}=0.2, \\beta=0$. Note: The first bin corresponds to...","name":"Table 56"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t57","@type":"Dataset","description":"Jet angularity $\\lambda_{\\alpha}$ for $\\alpha = 1$. $80&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;100$. For the \"trkeff\" and \"generator\" systematic uncertainty sources, the signed systematic...","name":"Table 57"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t58","@type":"Dataset","description":"Jet angularity $\\lambda_{\\alpha}$ for $\\alpha = 1.5$. $80&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;100$. For the \"trkeff\" and \"generator\" systematic uncertainty sources, the signed systematic...","name":"Table 58"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t59","@type":"Dataset","description":"Jet angularity $\\lambda_{\\alpha}$ for $\\alpha = 2$. $80&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;100$. For the \"trkeff\" and \"generator\" systematic uncertainty sources, the signed systematic...","name":"Table 59"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t60","@type":"Dataset","description":"Jet angularity $\\lambda_{\\alpha}$ for $\\alpha = 3$. $80&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;100$. For the \"trkeff\" and \"generator\" systematic uncertainty sources, the signed systematic...","name":"Table 60"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t61","@type":"Dataset","description":"Groomed jet angularity $\\lambda_{\\alpha,g}$ for $\\alpha = 1$. $80&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;100$, Soft Drop $z_{\\mathrm{cut}}=0.2, \\beta=0$. Note: The first bin corresponds to...","name":"Table 61"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t62","@type":"Dataset","description":"Groomed jet angularity $\\lambda_{\\alpha,g}$ for $\\alpha = 1.5$. $80&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;100$, Soft Drop $z_{\\mathrm{cut}}=0.2, \\beta=0$. Note: The first bin corresponds to...","name":"Table 62"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t63","@type":"Dataset","description":"Groomed jet angularity $\\lambda_{\\alpha,g}$ for $\\alpha = 2$. $80&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;100$, Soft Drop $z_{\\mathrm{cut}}=0.2, \\beta=0$. Note: The first bin corresponds to...","name":"Table 63"},{"@id":"https://doi.org/10.17182/hepdata.129149.v1/t64","@type":"Dataset","description":"Groomed jet angularity $\\lambda_{\\alpha,g}$ for $\\alpha = 3$. $80&lt;p_{\\mathrm{T}}^{\\mathrm{ch jet}}&lt;100$, Soft Drop $z_{\\mathrm{cut}}=0.2, \\beta=0$. Note: The first bin corresponds to...","name":"Table 64"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1891385?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/129149"}],"inLanguage":"en","name":"Measurements of the groomed and ungroomed jet angularities in pp collisions at $\\sqrt{s} = 5.02$ TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1891385?version=1","version":1}