cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.68902.v1/t5
title: "Table 5" of "Measurement of the spectral functions of axial-vector hadronic tau decays and determination of alpha(S)(M(tau)**2)."

description: Invariant mass-squared distributions of the decay $\tau^- \to 2\pi^- \pi^+ 2\pi^0 \nu_\tau$.

The error has been set to zero if it is smaller than the point size. A dash indicates a data point lying outside the plot range.
description: CERN-LEP. An analysis based on 124000 selected $\tau$ pairs recorded by the ALEPH detector at LEP provides the vector ($V$) and axial-vector ($A$) spectral functions of hadronic $\tau$ decays together with their total widths. This allows the evaluation of finite energy chiral sum rules that are weighted integrals over the $(V-A)$ spectral functions. In addition, a precise measurement of $\alpha_s$ along with a determination of non-perturbative contributions at the $\tau$ mass scale is performed. The experimentally and theoretically most robust determination of $\alpha_s(M_\tau^2)$ is obtained from the $(V+A)$ fit that yields $\alpha_s(M_\tau^2) = 0.334 \pm 0.022$ giving $\alpha_s(M_Z^2) = 0.1202 \pm 0.0027$ after the extrapolation to the mass of the Z boson. The approach of the Operator Product Expansion (OPE) is tested experimentally studying the evolution of the hadronic widths to masses smaller than the $\tau$ mass.

These numbers have been read from the plots in the paper.
DOI: 10.17182/hepdata.68902.v1/t6
title: "Table 6" of "Measurement of the spectral functions of axial-vector hadronic tau decays and determination of alpha(S)(M(tau)**2)."

description: Unfolded (physical) invariant mass-squared spectra of the $\tau$ final state $2\pi^- \pi^+ \nu_\tau$.

The error has been set to zero if it is smaller than the point size.
description: CERN-LEP. An analysis based on 124000 selected $\tau$ pairs recorded by the ALEPH detector at LEP provides the vector ($V$) and axial-vector ($A$) spectral functions of hadronic $\tau$ decays together with their total widths. This allows the evaluation of finite energy chiral sum rules that are weighted integrals over the $(V-A)$ spectral functions. In addition, a precise measurement of $\alpha_s$ along with a determination of non-perturbative contributions at the $\tau$ mass scale is performed. The experimentally and theoretically most robust determination of $\alpha_s(M_\tau^2)$ is obtained from the $(V+A)$ fit that yields $\alpha_s(M_\tau^2) = 0.334 \pm 0.022$ giving $\alpha_s(M_Z^2) = 0.1202 \pm 0.0027$ after the extrapolation to the mass of the Z boson. The approach of the Operator Product Expansion (OPE) is tested experimentally studying the evolution of the hadronic widths to masses smaller than the $\tau$ mass.

These numbers have been read from the plots in the paper.
DOI: 10.17182/hepdata.68902.v1/t7
title: "Table 7" of "Measurement of the spectral functions of axial-vector hadronic tau decays and determination of alpha(S)(M(tau)**2)."

description: Unfolded (physical) invariant mass-squared spectra of the $\tau$ final state $\pi^- 2\pi^0 \nu_\tau$.

The error has been set to zero if it is smaller than the point size.
description: CERN-LEP. An analysis based on 124000 selected $\tau$ pairs recorded by the ALEPH detector at LEP provides the vector ($V$) and axial-vector ($A$) spectral functions of hadronic $\tau$ decays together with their total widths. This allows the evaluation of finite energy chiral sum rules that are weighted integrals over the $(V-A)$ spectral functions. In addition, a precise measurement of $\alpha_s$ along with a determination of non-perturbative contributions at the $\tau$ mass scale is performed. The experimentally and theoretically most robust determination of $\alpha_s(M_\tau^2)$ is obtained from the $(V+A)$ fit that yields $\alpha_s(M_\tau^2) = 0.334 \pm 0.022$ giving $\alpha_s(M_Z^2) = 0.1202 \pm 0.0027$ after the extrapolation to the mass of the Z boson. The approach of the Operator Product Expansion (OPE) is tested experimentally studying the evolution of the hadronic widths to masses smaller than the $\tau$ mass.

These numbers have been read from the plots in the paper.
DOI: 10.17182/hepdata.68910.v1/t1
title: "Table 1" of "Measurement of the total cross section from elastic scattering in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector"

description: The measured total cross section, the first systematic error accounts for all experimental uncertainties and the second error for the extrapolation t--&gt;0.
description: CERN-LHC. A measurement of the total $pp$ cross section at the LHC at $\sqrt{s}=7$ TeV is presented. In a special run with high-$\beta^{\star}$ beam optics, an integrated luminosity of 80 $\mu$b$^{-1}$ was accumulated in order to measure the differential elastic cross section as a function of the Mandelstam momentum transfer variable $t$. The measurement is performed with the ALFA sub-detector of ATLAS. Using a fit to the differential elastic cross section in the $|t|$ range from 0.01 GeV$^2$ to 0.1 GeV$^2$ to extrapolate to $|t|\rightarrow 0$, the total cross section, $\sigma_{\mathrm{tot}}(pp\rightarrow X)$, is measured via the optical theorem to be: $$\sigma_{\mathrm{tot}}(pp\rightarrow X) = 95.35 \; \pm 0.38 \; ({\mbox{stat.}}) \pm 1.25 \; ({\mbox{exp.}}) \pm 0.37 \; (\mbox{extr.}) \; \mbox{mb},$$ where the first error is statistical, the second accounts for all experimental systematic uncertainties and the last is related to uncertainties in the extrapolation to $|t|\rightarrow 0$. In addition, the slope of the elastic cross section at small $|t|$ is determined to be $B = 19.73 \pm 0.14 \; ({\mbox{stat.}}) \pm 0.26 \; ({\mbox{syst.}}) \; \mbox{GeV}^{-2}$.
DOI: 10.17182/hepdata.68910.v1/t2
title: "Table 2" of "Measurement of the total cross section from elastic scattering in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector"

description: The nuclear slope of the differential eslastic cross section at small |t|, the first systematic error accounts for all experimental uncertainties and the second error for the extrapolation t--&gt;0.
description: CERN-LHC. A measurement of the total $pp$ cross section at the LHC at $\sqrt{s}=7$ TeV is presented. In a special run with high-$\beta^{\star}$ beam optics, an integrated luminosity of 80 $\mu$b$^{-1}$ was accumulated in order to measure the differential elastic cross section as a function of the Mandelstam momentum transfer variable $t$. The measurement is performed with the ALFA sub-detector of ATLAS. Using a fit to the differential elastic cross section in the $|t|$ range from 0.01 GeV$^2$ to 0.1 GeV$^2$ to extrapolate to $|t|\rightarrow 0$, the total cross section, $\sigma_{\mathrm{tot}}(pp\rightarrow X)$, is measured via the optical theorem to be: $$\sigma_{\mathrm{tot}}(pp\rightarrow X) = 95.35 \; \pm 0.38 \; ({\mbox{stat.}}) \pm 1.25 \; ({\mbox{exp.}}) \pm 0.37 \; (\mbox{extr.}) \; \mbox{mb},$$ where the first error is statistical, the second accounts for all experimental systematic uncertainties and the last is related to uncertainties in the extrapolation to $|t|\rightarrow 0$. In addition, the slope of the elastic cross section at small $|t|$ is determined to be $B = 19.73 \pm 0.14 \; ({\mbox{stat.}}) \pm 0.26 \; ({\mbox{syst.}}) \; \mbox{GeV}^{-2}$.
DOI: 10.17182/hepdata.68910.v1/t3
title: "Table 3" of "Measurement of the total cross section from elastic scattering in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector"

description: The Optical Point dsigma/(elastic)/dt(t--&gt;0), the total elastic cross section and the observed elastic cross section within the fiducial volume. The first systematic error accounts for all experimental uncertainties and the second error for the extrapolation t--&gt;0.
description: CERN-LHC. A measurement of the total $pp$ cross section at the LHC at $\sqrt{s}=7$ TeV is presented. In a special run with high-$\beta^{\star}$ beam optics, an integrated luminosity of 80 $\mu$b$^{-1}$ was accumulated in order to measure the differential elastic cross section as a function of the Mandelstam momentum transfer variable $t$. The measurement is performed with the ALFA sub-detector of ATLAS. Using a fit to the differential elastic cross section in the $|t|$ range from 0.01 GeV$^2$ to 0.1 GeV$^2$ to extrapolate to $|t|\rightarrow 0$, the total cross section, $\sigma_{\mathrm{tot}}(pp\rightarrow X)$, is measured via the optical theorem to be: $$\sigma_{\mathrm{tot}}(pp\rightarrow X) = 95.35 \; \pm 0.38 \; ({\mbox{stat.}}) \pm 1.25 \; ({\mbox{exp.}}) \pm 0.37 \; (\mbox{extr.}) \; \mbox{mb},$$ where the first error is statistical, the second accounts for all experimental systematic uncertainties and the last is related to uncertainties in the extrapolation to $|t|\rightarrow 0$. In addition, the slope of the elastic cross section at small $|t|$ is determined to be $B = 19.73 \pm 0.14 \; ({\mbox{stat.}}) \pm 0.26 \; ({\mbox{syst.}}) \; \mbox{GeV}^{-2}$.
DOI: 10.17182/hepdata.68910.v1/t4
title: "Table 4" of "Measurement of the total cross section from elastic scattering in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector"

description: The total inelastic cross section, the first systematic error accounts for all experimental uncertainties and the second error for the extrapolation t--&gt;0.
description: CERN-LHC. A measurement of the total $pp$ cross section at the LHC at $\sqrt{s}=7$ TeV is presented. In a special run with high-$\beta^{\star}$ beam optics, an integrated luminosity of 80 $\mu$b$^{-1}$ was accumulated in order to measure the differential elastic cross section as a function of the Mandelstam momentum transfer variable $t$. The measurement is performed with the ALFA sub-detector of ATLAS. Using a fit to the differential elastic cross section in the $|t|$ range from 0.01 GeV$^2$ to 0.1 GeV$^2$ to extrapolate to $|t|\rightarrow 0$, the total cross section, $\sigma_{\mathrm{tot}}(pp\rightarrow X)$, is measured via the optical theorem to be: $$\sigma_{\mathrm{tot}}(pp\rightarrow X) = 95.35 \; \pm 0.38 \; ({\mbox{stat.}}) \pm 1.25 \; ({\mbox{exp.}}) \pm 0.37 \; (\mbox{extr.}) \; \mbox{mb},$$ where the first error is statistical, the second accounts for all experimental systematic uncertainties and the last is related to uncertainties in the extrapolation to $|t|\rightarrow 0$. In addition, the slope of the elastic cross section at small $|t|$ is determined to be $B = 19.73 \pm 0.14 \; ({\mbox{stat.}}) \pm 0.26 \; ({\mbox{syst.}}) \; \mbox{GeV}^{-2}$.
DOI: 10.17182/hepdata.68910.v1/t6
title: "Table 6" of "Measurement of the total cross section from elastic scattering in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector"

description: The statistical covariance matrix for the differential elastic cross section.
description: CERN-LHC. A measurement of the total $pp$ cross section at the LHC at $\sqrt{s}=7$ TeV is presented. In a special run with high-$\beta^{\star}$ beam optics, an integrated luminosity of 80 $\mu$b$^{-1}$ was accumulated in order to measure the differential elastic cross section as a function of the Mandelstam momentum transfer variable $t$. The measurement is performed with the ALFA sub-detector of ATLAS. Using a fit to the differential elastic cross section in the $|t|$ range from 0.01 GeV$^2$ to 0.1 GeV$^2$ to extrapolate to $|t|\rightarrow 0$, the total cross section, $\sigma_{\mathrm{tot}}(pp\rightarrow X)$, is measured via the optical theorem to be: $$\sigma_{\mathrm{tot}}(pp\rightarrow X) = 95.35 \; \pm 0.38 \; ({\mbox{stat.}}) \pm 1.25 \; ({\mbox{exp.}}) \pm 0.37 \; (\mbox{extr.}) \; \mbox{mb},$$ where the first error is statistical, the second accounts for all experimental systematic uncertainties and the last is related to uncertainties in the extrapolation to $|t|\rightarrow 0$. In addition, the slope of the elastic cross section at small $|t|$ is determined to be $B = 19.73 \pm 0.14 \; ({\mbox{stat.}}) \pm 0.26 \; ({\mbox{syst.}}) \; \mbox{GeV}^{-2}$.
DOI: 10.17182/hepdata.68911.v1/t1
title: "Table 1" of "Measurement of charged jet production cross sections and nuclear modification in p-Pb collisions at $\sqrt{s_\rm{NN}} = 5.02$ TeV"

description: $p_\mathrm{T}$-differential production cross section of charged jets in p-Pb collisions at 5.02 TeV for $R = 0.2$ measured with the ALICE detector.
description: CERN-LHC-ALICE.
Charged jet production cross sections in p-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV measured with the ALICE detector at the LHC are presented. Using the anti-$k_T$ algorithm, jets have been reconstructed in the central rapidity region from charged particles with resolution parameters $R = 0.2$ and $R = 0.4$. The reconstructed jets have been corrected for detector effects and the underlying event background. To calculate the nuclear modification factor $R_\mathrm{pPb}$ of charged jets in p-Pb collisions, a pp reference was constructed by scaling previously measured charged jet spectra at $\sqrt{s} = 7$ TeV. In the transverse momentum range $20 \leq p_\mathrm{T,\;ch\;jet} \leq 120$ GeV/$c$, $R_\mathrm{pPb}$ is found to be consistent with unity, indicating the absence of strong nuclear matter effects on jet production. Major changes to the radial jet structure are probed via the ratio of jet production cross sections reconstructed with the two different resolution parameters. This ratio is found to be similar to the measurement in pp collisions at $\sqrt{s} = 7$ TeV and to the expectations from PYTHIA pp simulations and NLO pQCD calculations at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV.
DOI: 10.17182/hepdata.68911.v1/t2
title: "Table 2" of "Measurement of charged jet production cross sections and nuclear modification in p-Pb collisions at $\sqrt{s_\rm{NN}} = 5.02$ TeV"

description: $p_\mathrm{T}$-differential production cross section of charged jets in p-Pb collisions at 5.02 TeV for R = 0.2 calculated with a Lorentz-boosted NLO pQCD calculation using POWHEG+PYTHIA8 with CTEQ6.6+EPS09.
description: CERN-LHC-ALICE.
Charged jet production cross sections in p-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV measured with the ALICE detector at the LHC are presented. Using the anti-$k_T$ algorithm, jets have been reconstructed in the central rapidity region from charged particles with resolution parameters $R = 0.2$ and $R = 0.4$. The reconstructed jets have been corrected for detector effects and the underlying event background. To calculate the nuclear modification factor $R_\mathrm{pPb}$ of charged jets in p-Pb collisions, a pp reference was constructed by scaling previously measured charged jet spectra at $\sqrt{s} = 7$ TeV. In the transverse momentum range $20 \leq p_\mathrm{T,\;ch\;jet} \leq 120$ GeV/$c$, $R_\mathrm{pPb}$ is found to be consistent with unity, indicating the absence of strong nuclear matter effects on jet production. Major changes to the radial jet structure are probed via the ratio of jet production cross sections reconstructed with the two different resolution parameters. This ratio is found to be similar to the measurement in pp collisions at $\sqrt{s} = 7$ TeV and to the expectations from PYTHIA pp simulations and NLO pQCD calculations at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV.
DOI: 10.17182/hepdata.68911.v1/t3
title: "Table 3" of "Measurement of charged jet production cross sections and nuclear modification in p-Pb collisions at $\sqrt{s_\rm{NN}} = 5.02$ TeV"

description: $p_\mathrm{T}$-differential production cross section of charged jets in p-Pb collisions at 5.02 TeV for R = 0.2 measured with the ALICE detector. Eta-Interval 0.25 &lt; $\eta$ &lt; 0.65.
description: CERN-LHC-ALICE.
Charged jet production cross sections in p-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV measured with the ALICE detector at the LHC are presented. Using the anti-$k_T$ algorithm, jets have been reconstructed in the central rapidity region from charged particles with resolution parameters $R = 0.2$ and $R = 0.4$. The reconstructed jets have been corrected for detector effects and the underlying event background. To calculate the nuclear modification factor $R_\mathrm{pPb}$ of charged jets in p-Pb collisions, a pp reference was constructed by scaling previously measured charged jet spectra at $\sqrt{s} = 7$ TeV. In the transverse momentum range $20 \leq p_\mathrm{T,\;ch\;jet} \leq 120$ GeV/$c$, $R_\mathrm{pPb}$ is found to be consistent with unity, indicating the absence of strong nuclear matter effects on jet production. Major changes to the radial jet structure are probed via the ratio of jet production cross sections reconstructed with the two different resolution parameters. This ratio is found to be similar to the measurement in pp collisions at $\sqrt{s} = 7$ TeV and to the expectations from PYTHIA pp simulations and NLO pQCD calculations at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV.
DOI: 10.17182/hepdata.68911.v1/t4
title: "Table 4" of "Measurement of charged jet production cross sections and nuclear modification in p-Pb collisions at $\sqrt{s_\rm{NN}} = 5.02$ TeV"

description: $p_\mathrm{T}$-differential production cross section of charged jets in p-Pb collisions at 5.02 TeV for R = 0.2 measured with the ALICE detector. Eta-Interval -0.65 &lt; $\eta$ &lt; -0.25.
description: CERN-LHC-ALICE.
Charged jet production cross sections in p-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV measured with the ALICE detector at the LHC are presented. Using the anti-$k_T$ algorithm, jets have been reconstructed in the central rapidity region from charged particles with resolution parameters $R = 0.2$ and $R = 0.4$. The reconstructed jets have been corrected for detector effects and the underlying event background. To calculate the nuclear modification factor $R_\mathrm{pPb}$ of charged jets in p-Pb collisions, a pp reference was constructed by scaling previously measured charged jet spectra at $\sqrt{s} = 7$ TeV. In the transverse momentum range $20 \leq p_\mathrm{T,\;ch\;jet} \leq 120$ GeV/$c$, $R_\mathrm{pPb}$ is found to be consistent with unity, indicating the absence of strong nuclear matter effects on jet production. Major changes to the radial jet structure are probed via the ratio of jet production cross sections reconstructed with the two different resolution parameters. This ratio is found to be similar to the measurement in pp collisions at $\sqrt{s} = 7$ TeV and to the expectations from PYTHIA pp simulations and NLO pQCD calculations at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV.
DOI: 10.17182/hepdata.68911.v1/t5
title: "Table 5" of "Measurement of charged jet production cross sections and nuclear modification in p-Pb collisions at $\sqrt{s_\rm{NN}} = 5.02$ TeV"

description: $p_\mathrm{T}$-differential production cross section of charged jets in p-Pb collisions at 5.02 TeV for R = 0.4 measured with the ALICE detector.
description: CERN-LHC-ALICE.
Charged jet production cross sections in p-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV measured with the ALICE detector at the LHC are presented. Using the anti-$k_T$ algorithm, jets have been reconstructed in the central rapidity region from charged particles with resolution parameters $R = 0.2$ and $R = 0.4$. The reconstructed jets have been corrected for detector effects and the underlying event background. To calculate the nuclear modification factor $R_\mathrm{pPb}$ of charged jets in p-Pb collisions, a pp reference was constructed by scaling previously measured charged jet spectra at $\sqrt{s} = 7$ TeV. In the transverse momentum range $20 \leq p_\mathrm{T,\;ch\;jet} \leq 120$ GeV/$c$, $R_\mathrm{pPb}$ is found to be consistent with unity, indicating the absence of strong nuclear matter effects on jet production. Major changes to the radial jet structure are probed via the ratio of jet production cross sections reconstructed with the two different resolution parameters. This ratio is found to be similar to the measurement in pp collisions at $\sqrt{s} = 7$ TeV and to the expectations from PYTHIA pp simulations and NLO pQCD calculations at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV.
DOI: 10.17182/hepdata.68911.v1/t6
title: "Table 6" of "Measurement of charged jet production cross sections and nuclear modification in p-Pb collisions at $\sqrt{s_\rm{NN}} = 5.02$ TeV"

description: $p_\mathrm{T}$-differential production cross section of charged jets in p-Pb collisions at 5.02 TeV for R = 0.4 calculated with a Lorentz-boosted NLO pQCD calculation using POWHEG+PYTHIA8 with CTEQ6.6+EPS09.
description: CERN-LHC-ALICE.
Charged jet production cross sections in p-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV measured with the ALICE detector at the LHC are presented. Using the anti-$k_T$ algorithm, jets have been reconstructed in the central rapidity region from charged particles with resolution parameters $R = 0.2$ and $R = 0.4$. The reconstructed jets have been corrected for detector effects and the underlying event background. To calculate the nuclear modification factor $R_\mathrm{pPb}$ of charged jets in p-Pb collisions, a pp reference was constructed by scaling previously measured charged jet spectra at $\sqrt{s} = 7$ TeV. In the transverse momentum range $20 \leq p_\mathrm{T,\;ch\;jet} \leq 120$ GeV/$c$, $R_\mathrm{pPb}$ is found to be consistent with unity, indicating the absence of strong nuclear matter effects on jet production. Major changes to the radial jet structure are probed via the ratio of jet production cross sections reconstructed with the two different resolution parameters. This ratio is found to be similar to the measurement in pp collisions at $\sqrt{s} = 7$ TeV and to the expectations from PYTHIA pp simulations and NLO pQCD calculations at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV.
DOI: 10.17182/hepdata.68911.v1/t7
title: "Table 7" of "Measurement of charged jet production cross sections and nuclear modification in p-Pb collisions at $\sqrt{s_\rm{NN}} = 5.02$ TeV"

description: $p_\mathrm{T}$-differential production cross section of charged jets in p-Pb collisions at 5.02 TeV for R = 0.4 calculated with a Lorentz-boosted NLO pQCD calculation using POWHEG+PYTHIA8 with CTEQ6.6.
description: CERN-LHC-ALICE.
Charged jet production cross sections in p-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV measured with the ALICE detector at the LHC are presented. Using the anti-$k_T$ algorithm, jets have been reconstructed in the central rapidity region from charged particles with resolution parameters $R = 0.2$ and $R = 0.4$. The reconstructed jets have been corrected for detector effects and the underlying event background. To calculate the nuclear modification factor $R_\mathrm{pPb}$ of charged jets in p-Pb collisions, a pp reference was constructed by scaling previously measured charged jet spectra at $\sqrt{s} = 7$ TeV. In the transverse momentum range $20 \leq p_\mathrm{T,\;ch\;jet} \leq 120$ GeV/$c$, $R_\mathrm{pPb}$ is found to be consistent with unity, indicating the absence of strong nuclear matter effects on jet production. Major changes to the radial jet structure are probed via the ratio of jet production cross sections reconstructed with the two different resolution parameters. This ratio is found to be similar to the measurement in pp collisions at $\sqrt{s} = 7$ TeV and to the expectations from PYTHIA pp simulations and NLO pQCD calculations at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV.