{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.166442.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/3149790"}}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2026","description":"A simultaneous measurement of 25 N-subjettiness observables, forming an overcomplete basis for the 6-body kinematic phase space of emissions in a jet, is presented. The measurement is performed on large-radius (R=0.8), high-transverse-momentum jets: the more central jet in QCD dijet events and the leading jet in $\\mu$+jets $\\mathrm{t\\overline{t}}$ events wherein orthogonal regions enriched in Lorentz-boosted, hadronically decaying W bosons and top quarks are defined. The three data samples correspond to event selections with characteristically one-, two-, or three-prong jet topologies, arising from the showering and hadronization of a light-flavour quark or gluon, two quarks, or three quarks, respectively. For each selection, the combined one-dimensional distribution of all observables is unfolded to the particle level using a global binning scheme in which each unit-width, global bin maps to a particle-level bin in the physical range of each observable; a null bin of unit width separates between the different sub-distributions in the combined distribution. The unfolded combined distribution is normalized on a per-observable basis, such that the corresponding sub-distributions are normalized to unit area without explicitly assuming equal event yields per observable. Correspondingly, a block-diagonal Jacobian is used to transform the covariance matrices for the unfolded result to obtain the variance of the bins of the normalized, combined distribution, and to extract the particle-level correlations between bins of the individual observables presented in this data record. Particle-level differential cross-sections for the individual N-subjettiness observables are also provided. The relevant normalized sub-distributions for the individual N-subjettiness observables are extracted from the simultaneous unfolding, and rescaled by the (non-uniform) widths of the particle-level bins in the physical ranges of the observables in each event selection.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.166442.v1/t1","@type":"Dataset","description":"Fig. 7 (upper panel): The unfolded combined distribution of the overcomplete 6-body basis of N-subjettiness observables measured with the more...","name":"Unfolded 6-body, overcomplete N-subjettiness basis (QCD dijets)"},{"@id":"https://doi.org/10.17182/hepdata.166442.v1/t2","@type":"Dataset","description":"Fig. 28: Unfolded distribution of $\\tau_{1}^{(0.25)}$ extracted from the simultaneous unfolding. 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