cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.147275.v1/t24
title: "Figure 2 E3C divided by E2C 1410to1784 compare to NNLL_approx" of "Measurement of energy correlators inside jets and determination of the strong coupling $\alpha_\mathrm{S}(m_\mathrm{Z})$"

description: Unfolded E3C/E2C distributions in data compared to NLO+NNLL_approx predictions. Theoretial uncertainty in each bin is handled fully correlated as shape uncertainty. For the one-sided uncertainties, we symmetrize them when performing the fit.
description: We measure the two-point and three-point energy correlator jet substructure observables (E2C and E3C), using LHC 13 TeV data collected by the CMS experiment.The jets are clustered by anti-$k_\mathrm{t}$ algorithm with $R=0.4$ in a phase space region with jet $p_\mathrm{T}$ from 97 GeV up to 1.8 TeV and $|y|&lt;2.1$.The E2C and E3C distribution are measured in multiple jet transverse momentum regions, they show a sharp transition from the noninteger scaling behavior charaterizing the quantum interactions of quarks and gluons to an integer power law reflective of classical noninteracting hadrons.The ratio of E3C/E2C is directly proportional to the strong coupling constant $\alpha_S$, and the slopes of the ratio distribution consistent with the expected decrease of $\alpha_S$ with increasing energy due to asymptotic freedom.The ratio between E3C and E2C are compared to theoretical predictions with all-orders resummation at next-to-next-to-leading logarithmic accuracy matched to a fixed-order next-to-leading order calculation, yielding an $\alpha_S (m_Z)$ value of $0.1229^{+0.0040}_{-0.0050}$.This is the most precise extraction of $\alpha_S (m_Z)$ using jet substructure observables to date.
DOI: 10.17182/hepdata.147275.v1/t25
title: "Figure 2 Fitted slope of E3C divided by E2C data distribution" of "Measurement of energy correlators inside jets and determination of the strong coupling $\alpha_\mathrm{S}(m_\mathrm{Z})$"

description: The fitted slopes of the E3C/E2C data distributions as a function of jet pt are used to illustrate the dependency of alphas on jet pt.
description: We measure the two-point and three-point energy correlator jet substructure observables (E2C and E3C), using LHC 13 TeV data collected by the CMS experiment.The jets are clustered by anti-$k_\mathrm{t}$ algorithm with $R=0.4$ in a phase space region with jet $p_\mathrm{T}$ from 97 GeV up to 1.8 TeV and $|y|&lt;2.1$.The E2C and E3C distribution are measured in multiple jet transverse momentum regions, they show a sharp transition from the noninteger scaling behavior charaterizing the quantum interactions of quarks and gluons to an integer power law reflective of classical noninteracting hadrons.The ratio of E3C/E2C is directly proportional to the strong coupling constant $\alpha_S$, and the slopes of the ratio distribution consistent with the expected decrease of $\alpha_S$ with increasing energy due to asymptotic freedom.The ratio between E3C and E2C are compared to theoretical predictions with all-orders resummation at next-to-next-to-leading logarithmic accuracy matched to a fixed-order next-to-leading order calculation, yielding an $\alpha_S (m_Z)$ value of $0.1229^{+0.0040}_{-0.0050}$.This is the most precise extraction of $\alpha_S (m_Z)$ using jet substructure observables to date.
DOI: 10.17182/hepdata.147275.v1/t26
title: "Supplementary E3C divided by E2C 97to220 compare to MC" of "Measurement of energy correlators inside jets and determination of the strong coupling $\alpha_\mathrm{S}(m_\mathrm{Z})$"

description: Unfolded E3C/E2C distributions in data compared to MC predictions.
description: We measure the two-point and three-point energy correlator jet substructure observables (E2C and E3C), using LHC 13 TeV data collected by the CMS experiment.The jets are clustered by anti-$k_\mathrm{t}$ algorithm with $R=0.4$ in a phase space region with jet $p_\mathrm{T}$ from 97 GeV up to 1.8 TeV and $|y|&lt;2.1$.The E2C and E3C distribution are measured in multiple jet transverse momentum regions, they show a sharp transition from the noninteger scaling behavior charaterizing the quantum interactions of quarks and gluons to an integer power law reflective of classical noninteracting hadrons.The ratio of E3C/E2C is directly proportional to the strong coupling constant $\alpha_S$, and the slopes of the ratio distribution consistent with the expected decrease of $\alpha_S$ with increasing energy due to asymptotic freedom.The ratio between E3C and E2C are compared to theoretical predictions with all-orders resummation at next-to-next-to-leading logarithmic accuracy matched to a fixed-order next-to-leading order calculation, yielding an $\alpha_S (m_Z)$ value of $0.1229^{+0.0040}_{-0.0050}$.This is the most precise extraction of $\alpha_S (m_Z)$ using jet substructure observables to date.
DOI: 10.17182/hepdata.147275.v1/t27
title: "Supplementary E3C divided by E2C 220to330 compare to MC" of "Measurement of energy correlators inside jets and determination of the strong coupling $\alpha_\mathrm{S}(m_\mathrm{Z})$"

description: Unfolded E3C/E2C distributions in data compared to MC predictions.
description: We measure the two-point and three-point energy correlator jet substructure observables (E2C and E3C), using LHC 13 TeV data collected by the CMS experiment.The jets are clustered by anti-$k_\mathrm{t}$ algorithm with $R=0.4$ in a phase space region with jet $p_\mathrm{T}$ from 97 GeV up to 1.8 TeV and $|y|&lt;2.1$.The E2C and E3C distribution are measured in multiple jet transverse momentum regions, they show a sharp transition from the noninteger scaling behavior charaterizing the quantum interactions of quarks and gluons to an integer power law reflective of classical noninteracting hadrons.The ratio of E3C/E2C is directly proportional to the strong coupling constant $\alpha_S$, and the slopes of the ratio distribution consistent with the expected decrease of $\alpha_S$ with increasing energy due to asymptotic freedom.The ratio between E3C and E2C are compared to theoretical predictions with all-orders resummation at next-to-next-to-leading logarithmic accuracy matched to a fixed-order next-to-leading order calculation, yielding an $\alpha_S (m_Z)$ value of $0.1229^{+0.0040}_{-0.0050}$.This is the most precise extraction of $\alpha_S (m_Z)$ using jet substructure observables to date.
DOI: 10.17182/hepdata.147275.v1/t28
title: "Supplementary E3C divided by E2C 330to468 compare to MC" of "Measurement of energy correlators inside jets and determination of the strong coupling $\alpha_\mathrm{S}(m_\mathrm{Z})$"

description: Unfolded E3C/E2C distributions in data compared to MC predictions.
description: We measure the two-point and three-point energy correlator jet substructure observables (E2C and E3C), using LHC 13 TeV data collected by the CMS experiment.The jets are clustered by anti-$k_\mathrm{t}$ algorithm with $R=0.4$ in a phase space region with jet $p_\mathrm{T}$ from 97 GeV up to 1.8 TeV and $|y|&lt;2.1$.The E2C and E3C distribution are measured in multiple jet transverse momentum regions, they show a sharp transition from the noninteger scaling behavior charaterizing the quantum interactions of quarks and gluons to an integer power law reflective of classical noninteracting hadrons.The ratio of E3C/E2C is directly proportional to the strong coupling constant $\alpha_S$, and the slopes of the ratio distribution consistent with the expected decrease of $\alpha_S$ with increasing energy due to asymptotic freedom.The ratio between E3C and E2C are compared to theoretical predictions with all-orders resummation at next-to-next-to-leading logarithmic accuracy matched to a fixed-order next-to-leading order calculation, yielding an $\alpha_S (m_Z)$ value of $0.1229^{+0.0040}_{-0.0050}$.This is the most precise extraction of $\alpha_S (m_Z)$ using jet substructure observables to date.
DOI: 10.17182/hepdata.147275.v1/t29
title: "Supplementary E3C divided by E2C 468to638 compare to MC" of "Measurement of energy correlators inside jets and determination of the strong coupling $\alpha_\mathrm{S}(m_\mathrm{Z})$"

description: Unfolded E3C/E2C distributions in data compared to MC predictions.
description: We measure the two-point and three-point energy correlator jet substructure observables (E2C and E3C), using LHC 13 TeV data collected by the CMS experiment.The jets are clustered by anti-$k_\mathrm{t}$ algorithm with $R=0.4$ in a phase space region with jet $p_\mathrm{T}$ from 97 GeV up to 1.8 TeV and $|y|&lt;2.1$.The E2C and E3C distribution are measured in multiple jet transverse momentum regions, they show a sharp transition from the noninteger scaling behavior charaterizing the quantum interactions of quarks and gluons to an integer power law reflective of classical noninteracting hadrons.The ratio of E3C/E2C is directly proportional to the strong coupling constant $\alpha_S$, and the slopes of the ratio distribution consistent with the expected decrease of $\alpha_S$ with increasing energy due to asymptotic freedom.The ratio between E3C and E2C are compared to theoretical predictions with all-orders resummation at next-to-next-to-leading logarithmic accuracy matched to a fixed-order next-to-leading order calculation, yielding an $\alpha_S (m_Z)$ value of $0.1229^{+0.0040}_{-0.0050}$.This is the most precise extraction of $\alpha_S (m_Z)$ using jet substructure observables to date.
DOI: 10.17182/hepdata.147275.v1/t30
title: "Supplementary E3C divided by E2C 638to846 compare to MC" of "Measurement of energy correlators inside jets and determination of the strong coupling $\alpha_\mathrm{S}(m_\mathrm{Z})$"

description: Unfolded E3C/E2C distributions in data compared to MC predictions.
description: We measure the two-point and three-point energy correlator jet substructure observables (E2C and E3C), using LHC 13 TeV data collected by the CMS experiment.The jets are clustered by anti-$k_\mathrm{t}$ algorithm with $R=0.4$ in a phase space region with jet $p_\mathrm{T}$ from 97 GeV up to 1.8 TeV and $|y|&lt;2.1$.The E2C and E3C distribution are measured in multiple jet transverse momentum regions, they show a sharp transition from the noninteger scaling behavior charaterizing the quantum interactions of quarks and gluons to an integer power law reflective of classical noninteracting hadrons.The ratio of E3C/E2C is directly proportional to the strong coupling constant $\alpha_S$, and the slopes of the ratio distribution consistent with the expected decrease of $\alpha_S$ with increasing energy due to asymptotic freedom.The ratio between E3C and E2C are compared to theoretical predictions with all-orders resummation at next-to-next-to-leading logarithmic accuracy matched to a fixed-order next-to-leading order calculation, yielding an $\alpha_S (m_Z)$ value of $0.1229^{+0.0040}_{-0.0050}$.This is the most precise extraction of $\alpha_S (m_Z)$ using jet substructure observables to date.
DOI: 10.17182/hepdata.147275.v1/t31
title: "Supplementary E3C divided by E2C 846to1101 compare to MC" of "Measurement of energy correlators inside jets and determination of the strong coupling $\alpha_\mathrm{S}(m_\mathrm{Z})$"

description: Unfolded E3C/E2C distributions in data compared to MC predictions.
description: We measure the two-point and three-point energy correlator jet substructure observables (E2C and E3C), using LHC 13 TeV data collected by the CMS experiment.The jets are clustered by anti-$k_\mathrm{t}$ algorithm with $R=0.4$ in a phase space region with jet $p_\mathrm{T}$ from 97 GeV up to 1.8 TeV and $|y|&lt;2.1$.The E2C and E3C distribution are measured in multiple jet transverse momentum regions, they show a sharp transition from the noninteger scaling behavior charaterizing the quantum interactions of quarks and gluons to an integer power law reflective of classical noninteracting hadrons.The ratio of E3C/E2C is directly proportional to the strong coupling constant $\alpha_S$, and the slopes of the ratio distribution consistent with the expected decrease of $\alpha_S$ with increasing energy due to asymptotic freedom.The ratio between E3C and E2C are compared to theoretical predictions with all-orders resummation at next-to-next-to-leading logarithmic accuracy matched to a fixed-order next-to-leading order calculation, yielding an $\alpha_S (m_Z)$ value of $0.1229^{+0.0040}_{-0.0050}$.This is the most precise extraction of $\alpha_S (m_Z)$ using jet substructure observables to date.
DOI: 10.17182/hepdata.147275.v1/t32
title: "Supplementary E3C divided by E2C 1101to1410 compare to MC" of "Measurement of energy correlators inside jets and determination of the strong coupling $\alpha_\mathrm{S}(m_\mathrm{Z})$"

description: Unfolded E3C/E2C distributions in data compared to MC predictions.
description: We measure the two-point and three-point energy correlator jet substructure observables (E2C and E3C), using LHC 13 TeV data collected by the CMS experiment.The jets are clustered by anti-$k_\mathrm{t}$ algorithm with $R=0.4$ in a phase space region with jet $p_\mathrm{T}$ from 97 GeV up to 1.8 TeV and $|y|&lt;2.1$.The E2C and E3C distribution are measured in multiple jet transverse momentum regions, they show a sharp transition from the noninteger scaling behavior charaterizing the quantum interactions of quarks and gluons to an integer power law reflective of classical noninteracting hadrons.The ratio of E3C/E2C is directly proportional to the strong coupling constant $\alpha_S$, and the slopes of the ratio distribution consistent with the expected decrease of $\alpha_S$ with increasing energy due to asymptotic freedom.The ratio between E3C and E2C are compared to theoretical predictions with all-orders resummation at next-to-next-to-leading logarithmic accuracy matched to a fixed-order next-to-leading order calculation, yielding an $\alpha_S (m_Z)$ value of $0.1229^{+0.0040}_{-0.0050}$.This is the most precise extraction of $\alpha_S (m_Z)$ using jet substructure observables to date.
DOI: 10.17182/hepdata.147275.v1/t33
title: "Supplementary E3C divided by E2C 1410to1784 compare to MC" of "Measurement of energy correlators inside jets and determination of the strong coupling $\alpha_\mathrm{S}(m_\mathrm{Z})$"

description: Unfolded E3C/E2C distributions in data compared to MC predictions.
description: We measure the two-point and three-point energy correlator jet substructure observables (E2C and E3C), using LHC 13 TeV data collected by the CMS experiment.The jets are clustered by anti-$k_\mathrm{t}$ algorithm with $R=0.4$ in a phase space region with jet $p_\mathrm{T}$ from 97 GeV up to 1.8 TeV and $|y|&lt;2.1$.The E2C and E3C distribution are measured in multiple jet transverse momentum regions, they show a sharp transition from the noninteger scaling behavior charaterizing the quantum interactions of quarks and gluons to an integer power law reflective of classical noninteracting hadrons.The ratio of E3C/E2C is directly proportional to the strong coupling constant $\alpha_S$, and the slopes of the ratio distribution consistent with the expected decrease of $\alpha_S$ with increasing energy due to asymptotic freedom.The ratio between E3C and E2C are compared to theoretical predictions with all-orders resummation at next-to-next-to-leading logarithmic accuracy matched to a fixed-order next-to-leading order calculation, yielding an $\alpha_S (m_Z)$ value of $0.1229^{+0.0040}_{-0.0050}$.This is the most precise extraction of $\alpha_S (m_Z)$ using jet substructure observables to date.
DOI: 10.17182/hepdata.147275.v1/t34
title: "Supplementary chi2 scan" of "Measurement of energy correlators inside jets and determination of the strong coupling $\alpha_\mathrm{S}(m_\mathrm{Z})$"

description: The chi2 scan result using eq.3 for different alphas.
description: We measure the two-point and three-point energy correlator jet substructure observables (E2C and E3C), using LHC 13 TeV data collected by the CMS experiment.The jets are clustered by anti-$k_\mathrm{t}$ algorithm with $R=0.4$ in a phase space region with jet $p_\mathrm{T}$ from 97 GeV up to 1.8 TeV and $|y|&lt;2.1$.The E2C and E3C distribution are measured in multiple jet transverse momentum regions, they show a sharp transition from the noninteger scaling behavior charaterizing the quantum interactions of quarks and gluons to an integer power law reflective of classical noninteracting hadrons.The ratio of E3C/E2C is directly proportional to the strong coupling constant $\alpha_S$, and the slopes of the ratio distribution consistent with the expected decrease of $\alpha_S$ with increasing energy due to asymptotic freedom.The ratio between E3C and E2C are compared to theoretical predictions with all-orders resummation at next-to-next-to-leading logarithmic accuracy matched to a fixed-order next-to-leading order calculation, yielding an $\alpha_S (m_Z)$ value of $0.1229^{+0.0040}_{-0.0050}$.This is the most precise extraction of $\alpha_S (m_Z)$ using jet substructure observables to date.
DOI: 10.17182/hepdata.147275.v1/t35
title: "Supplementary E2C stat correlation matrix" of "Measurement of energy correlators inside jets and determination of the strong coupling $\alpha_\mathrm{S}(m_\mathrm{Z})$"

description: The correlation matrix is composed by 10 jet pt region, each region is represented by a block in the plot. Inside each block, there are 22 xL bins same as the E2C, E3C and E3C/E2C distributions. Therefore, the x and y bins of the correlation matrix is given by, binNumber = pT_index * 22 + xL_index.
description: We measure the two-point and three-point energy correlator jet substructure observables (E2C and E3C), using LHC 13 TeV data collected by the CMS experiment.The jets are clustered by anti-$k_\mathrm{t}$ algorithm with $R=0.4$ in a phase space region with jet $p_\mathrm{T}$ from 97 GeV up to 1.8 TeV and $|y|&lt;2.1$.The E2C and E3C distribution are measured in multiple jet transverse momentum regions, they show a sharp transition from the noninteger scaling behavior charaterizing the quantum interactions of quarks and gluons to an integer power law reflective of classical noninteracting hadrons.The ratio of E3C/E2C is directly proportional to the strong coupling constant $\alpha_S$, and the slopes of the ratio distribution consistent with the expected decrease of $\alpha_S$ with increasing energy due to asymptotic freedom.The ratio between E3C and E2C are compared to theoretical predictions with all-orders resummation at next-to-next-to-leading logarithmic accuracy matched to a fixed-order next-to-leading order calculation, yielding an $\alpha_S (m_Z)$ value of $0.1229^{+0.0040}_{-0.0050}$.This is the most precise extraction of $\alpha_S (m_Z)$ using jet substructure observables to date.
DOI: 10.17182/hepdata.147275.v1/t36
title: "Supplementary E3C stat correlation matrix" of "Measurement of energy correlators inside jets and determination of the strong coupling $\alpha_\mathrm{S}(m_\mathrm{Z})$"

description: The correlation matrix is composed by 10 jet pt region, each region is represented by a block in the plot. Inside each block, there are 22 xL bins same as the E2C, E3C and E3C/E2C distributions. Therefore, the x and y bins of the correlation matrix is given by, binNumber = pT_index * 22 + xL_index.
description: We measure the two-point and three-point energy correlator jet substructure observables (E2C and E3C), using LHC 13 TeV data collected by the CMS experiment.The jets are clustered by anti-$k_\mathrm{t}$ algorithm with $R=0.4$ in a phase space region with jet $p_\mathrm{T}$ from 97 GeV up to 1.8 TeV and $|y|&lt;2.1$.The E2C and E3C distribution are measured in multiple jet transverse momentum regions, they show a sharp transition from the noninteger scaling behavior charaterizing the quantum interactions of quarks and gluons to an integer power law reflective of classical noninteracting hadrons.The ratio of E3C/E2C is directly proportional to the strong coupling constant $\alpha_S$, and the slopes of the ratio distribution consistent with the expected decrease of $\alpha_S$ with increasing energy due to asymptotic freedom.The ratio between E3C and E2C are compared to theoretical predictions with all-orders resummation at next-to-next-to-leading logarithmic accuracy matched to a fixed-order next-to-leading order calculation, yielding an $\alpha_S (m_Z)$ value of $0.1229^{+0.0040}_{-0.0050}$.This is the most precise extraction of $\alpha_S (m_Z)$ using jet substructure observables to date.
DOI: 10.17182/hepdata.147275.v1/t37
title: "Supplementary E3C divided by E2C correlation matrix" of "Measurement of energy correlators inside jets and determination of the strong coupling $\alpha_\mathrm{S}(m_\mathrm{Z})$"

description: The correlation matrix is composed by 10 jet pt region, each region is represented by a block in the plot. Inside each block, there are 22 xL bins same as the E2C, E3C and E3C/E2C distributions. Therefore, the x and y bins of the correlation matrix is given by, binNumber = pT_index * 22 + xL_index.
description: We measure the two-point and three-point energy correlator jet substructure observables (E2C and E3C), using LHC 13 TeV data collected by the CMS experiment.The jets are clustered by anti-$k_\mathrm{t}$ algorithm with $R=0.4$ in a phase space region with jet $p_\mathrm{T}$ from 97 GeV up to 1.8 TeV and $|y|&lt;2.1$.The E2C and E3C distribution are measured in multiple jet transverse momentum regions, they show a sharp transition from the noninteger scaling behavior charaterizing the quantum interactions of quarks and gluons to an integer power law reflective of classical noninteracting hadrons.The ratio of E3C/E2C is directly proportional to the strong coupling constant $\alpha_S$, and the slopes of the ratio distribution consistent with the expected decrease of $\alpha_S$ with increasing energy due to asymptotic freedom.The ratio between E3C and E2C are compared to theoretical predictions with all-orders resummation at next-to-next-to-leading logarithmic accuracy matched to a fixed-order next-to-leading order calculation, yielding an $\alpha_S (m_Z)$ value of $0.1229^{+0.0040}_{-0.0050}$.This is the most precise extraction of $\alpha_S (m_Z)$ using jet substructure observables to date.
DOI: 10.17182/hepdata.147275.v1/t38
title: "Supplementary E2C energy weight binning" of "Measurement of energy correlators inside jets and determination of the strong coupling $\alpha_\mathrm{S}(m_\mathrm{Z})$"

description: The energy weight of E2C as defined in eq.1 in the paper is used in the unfolding, the binning is listed in this table.
description: We measure the two-point and three-point energy correlator jet substructure observables (E2C and E3C), using LHC 13 TeV data collected by the CMS experiment.The jets are clustered by anti-$k_\mathrm{t}$ algorithm with $R=0.4$ in a phase space region with jet $p_\mathrm{T}$ from 97 GeV up to 1.8 TeV and $|y|&lt;2.1$.The E2C and E3C distribution are measured in multiple jet transverse momentum regions, they show a sharp transition from the noninteger scaling behavior charaterizing the quantum interactions of quarks and gluons to an integer power law reflective of classical noninteracting hadrons.The ratio of E3C/E2C is directly proportional to the strong coupling constant $\alpha_S$, and the slopes of the ratio distribution consistent with the expected decrease of $\alpha_S$ with increasing energy due to asymptotic freedom.The ratio between E3C and E2C are compared to theoretical predictions with all-orders resummation at next-to-next-to-leading logarithmic accuracy matched to a fixed-order next-to-leading order calculation, yielding an $\alpha_S (m_Z)$ value of $0.1229^{+0.0040}_{-0.0050}$.This is the most precise extraction of $\alpha_S (m_Z)$ using jet substructure observables to date.