cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.147275.v1/t11
title: "Figure 1 E3C 330to468" of "Measurement of energy correlators inside jets and determination of the strong coupling $\alpha_\mathrm{S}(m_\mathrm{Z})$"

description: Unfolded E3C 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/t12
title: "Figure 1 E3C 468to638" of "Measurement of energy correlators inside jets and determination of the strong coupling $\alpha_\mathrm{S}(m_\mathrm{Z})$"

description: Unfolded E3C 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/t13
title: "Figure 1 E3C 638to846" of "Measurement of energy correlators inside jets and determination of the strong coupling $\alpha_\mathrm{S}(m_\mathrm{Z})$"

description: Unfolded E3C 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/t15
title: "Figure 1 E3C 1101to1410" of "Measurement of energy correlators inside jets and determination of the strong coupling $\alpha_\mathrm{S}(m_\mathrm{Z})$"

description: Unfolded E3C 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/t8
title: "Figure 1 E2C 1410to1784" of "Measurement of energy correlators inside jets and determination of the strong coupling $\alpha_\mathrm{S}(m_\mathrm{Z})$"

description: Unfolded 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/t9
title: "Figure 1 E3C 97to220" of "Measurement of energy correlators inside jets and determination of the strong coupling $\alpha_\mathrm{S}(m_\mathrm{Z})$"

description: Unfolded E3C 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/t14
title: "Figure 1 E3C 846to1101" of "Measurement of energy correlators inside jets and determination of the strong coupling $\alpha_\mathrm{S}(m_\mathrm{Z})$"

description: Unfolded E3C 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/t16
title: "Figure 1 E3C 1410to1784" of "Measurement of energy correlators inside jets and determination of the strong coupling $\alpha_\mathrm{S}(m_\mathrm{Z})$"

description: Unfolded E3C 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/t17
title: "Figure 2 E3C divided by E2C 97to220 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/t18
title: "Figure 2 E3C divided by E2C 220to330 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/t19
title: "Figure 2 E3C divided by E2C 330to468 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/t20
title: "Figure 2 E3C divided by E2C 468to638 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/t21
title: "Figure 2 E3C divided by E2C 638to846 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/t22
title: "Figure 2 E3C divided by E2C 846to1101 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/t23
title: "Figure 2 E3C divided by E2C 1101to1410 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.