cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.68011.v1/t1
title: "Table 1" of "K0 production in one prong tau decays"

description: Invariant mass distribution for the $K^0\pi$ system data. The numbers have been read from the plot in the paper.
description: CERN-LEP. From a sample of about 75000 $\tau$ decays identified with the ALEPH detector, $K^0$ production in 1-prong hadronic decays is investigated by tagging the $K^0_L$ component in a hadronic calorimeter. Results are given for the final states $\nu_{\tau}h^-K^0$ and $\nu_{\tau}h^-\pi^0K^0$ where the $h^-$ is separated into $\pi$ and $K$ contributions by means of the $dE/dx$ measurement in the central detector. The resulting branching ratios are:
$$\begin{eqnarray}
(B\tau\to\nu_{\tau}\pi^-K^0) = (0.88\pm0.14\pm0.09)\%,\\
(B\tau\to\nu_{\tau}K^-K^0) = (0.29\pm0.12\pm0.03)\%,\\
(B\tau\to\nu_{\tau}\pi^-\pi^0K^0) = (0.33\pm0.14\pm0.07)\%\\
\mathrm{and}\quad
(B\tau\to\nu_{\tau}K^-\pi^0K^0) = (0.05\pm0.05\pm0.01)\%.
\end{eqnarray}$$.
The $K^*$ decay rate in the $K^0\pi$ channel agrees with that in the $K\pi^0$ mode: the combined value for the branching ratio is $(B\tau\to\nu_{\tau}K^{*^-}) = (1.45\pm0.13\pm0.11)\%$.
DOI: 10.17182/hepdata.68012.v1/t1
title: "Table 1" of "One prong tau decays into charged kaons"

description: Invariant mass distribution of the $K\pi^0$ final state, as obtained from a $dE/dx$ fit in each mass bin. The numbers have been read from the plot in the paper, with the errors simply set to zero if they are smaller than the point size.
description: CERN-LEP. From a sample of about 75000 $\tau$ decays measured in the ALEPH detector, 1-prong charged kaon decays are identified by the $dE/dx$ measurements in the central detector. The resulting branching ratios for the inclusive and exclusive modes are:
$$\begin{eqnarray}
B(\tau\to\nu_{\tau}K^-\geq0\pi^0\geq0K^0) = (1.60\pm0.07\pm0.12)\%,\\
B(\tau\to\nu_{\tau}K^-) = (0.64\pm0.05\pm0.05)\%,\\
B(\tau\to\nu_{\tau}K^-\pi^0) = (0.53\pm0.05\pm0.07)\%\\
\mathrm{and}\quad
B(\tau\to\nu_{\tau}K^-\pi^0\pi^0) = (0.04\pm0.03\pm0.02)\%.
\end{eqnarray}$$
Exclusive modes are corrected for measured $K_L^0$ production. The rate for $\tau\to\nu_{\tau}K^-$ agrees well with the prediction based on $\tau-\mu$ universality.
DOI: 10.17182/hepdata.68015.v1/t1
title: "Table 1" of "Soft and hard interactions in p anti-p collisions at s**(1/2) = 1800-GeV and 630-GeV"

description: Charged multiplicity at $\sqrt{s} = 630~\text{GeV}$, $|\eta| &lt; 1$, $p_T &gt; 0.4~\text{GeV}$.
description: We present a study of ppbar collisions at (s)=1800 and 630 GeV collected using a minimum bias trigger by the CDF experiment in which the data set is divided into two classes corresponding to ``soft and ``hard interactions. For each subsample, the analysis includes measurements of the multiplicity, transverse momentum (pT) spectrum, and the average pT and event-by-event pT dispersion as a function of multiplicity. A comparison of results shows distinct differences in the behavior of the two samples as a function of the center of mass (c.m.) energy. We find evidence that the properties of the soft sample are invariant as a function of c.m. energy.
Data taken from the RIVET analysis code.
DOI: 10.17182/hepdata.68015.v1/t2
title: "Table 2" of "Soft and hard interactions in p anti-p collisions at s**(1/2) = 1800-GeV and 630-GeV"

description: Charged multiplicity at $\sqrt{s} = 1800~\text{GeV}$, $|\eta| &lt; 1$, $p_T &gt; 0.4~\text{GeV}$.
description: We present a study of ppbar collisions at (s)=1800 and 630 GeV collected using a minimum bias trigger by the CDF experiment in which the data set is divided into two classes corresponding to ``soft and ``hard interactions. For each subsample, the analysis includes measurements of the multiplicity, transverse momentum (pT) spectrum, and the average pT and event-by-event pT dispersion as a function of multiplicity. A comparison of results shows distinct differences in the behavior of the two samples as a function of the center of mass (c.m.) energy. We find evidence that the properties of the soft sample are invariant as a function of c.m. energy.
Data taken from the RIVET analysis code.
DOI: 10.17182/hepdata.68015.v1/t3
title: "Table 3" of "Soft and hard interactions in p anti-p collisions at s**(1/2) = 1800-GeV and 630-GeV"

description: $\langle p_\perp \rangle$ vs. multiplicity at $\sqrt{s} = 630~\text{GeV}$, $|\eta| &lt; 1$, $p_T &gt; 0.4~\text{GeV}$.
description: We present a study of ppbar collisions at (s)=1800 and 630 GeV collected using a minimum bias trigger by the CDF experiment in which the data set is divided into two classes corresponding to ``soft and ``hard interactions. For each subsample, the analysis includes measurements of the multiplicity, transverse momentum (pT) spectrum, and the average pT and event-by-event pT dispersion as a function of multiplicity. A comparison of results shows distinct differences in the behavior of the two samples as a function of the center of mass (c.m.) energy. We find evidence that the properties of the soft sample are invariant as a function of c.m. energy.
Data taken from the RIVET analysis code.
DOI: 10.17182/hepdata.68015.v1/t4
title: "Table 4" of "Soft and hard interactions in p anti-p collisions at s**(1/2) = 1800-GeV and 630-GeV"

description: $\langle p_\perp \rangle$ vs. multiplicity at $\sqrt{s} = 1800~\text{GeV}$, $|\eta| &lt; 1$, $p_T &gt; 0.4~\text{GeV}$.
description: We present a study of ppbar collisions at (s)=1800 and 630 GeV collected using a minimum bias trigger by the CDF experiment in which the data set is divided into two classes corresponding to ``soft and ``hard interactions. For each subsample, the analysis includes measurements of the multiplicity, transverse momentum (pT) spectrum, and the average pT and event-by-event pT dispersion as a function of multiplicity. A comparison of results shows distinct differences in the behavior of the two samples as a function of the center of mass (c.m.) energy. We find evidence that the properties of the soft sample are invariant as a function of c.m. energy.
Data taken from the RIVET analysis code.
DOI: 10.17182/hepdata.68020.v1/t1
title: "Table 1" of "Measurement of the ratio of inclusive jet cross sections using the anti-kt algorithm with radius parameters R = 0.5 and 0.7 in pp collisions at sqrt(s) = 7 TeV"

description: Inclusive Jet cross section with R = 0.5 in the rapidity bin 0 &lt; |y| &lt; 0.5. The total uncorrelated uncertainty includes statistical one and systematic uncorrelated. The total systematic uncertainty includes all other sources, especially the luminosity uncertainty of 2.2%. The total error can be obtained as a quadratic sum of uncorrelated and correlated one. The NP correction can be used to scale theory prediction to compare to data at particle level.
description: CERN-LHC. Measurements of the inclusive jet cross section with the anti-kt clustering algorithm are presented for two radius parameters, R=0.5 and 0.7. They are based on data from LHC proton-proton collisions at $\sqrt{s}$ = 7 TeV corresponding to an integrated luminosity of 5.0 inverse femtobarns collected with the CMS detector in 2011. The ratio of these two measurements is obtained as a function of the rapidity and transverse momentum of the jets. Significant discrepancies are found comparing the data to leading-order simulations and to fixed-order calculations at next-to-leading order, corrected for nonperturbative effects, whereas simulations with next-to-leading-order matrix elements matched to parton showers describe the data best.
DOI: 10.17182/hepdata.68020.v1/t2
title: "Table 2" of "Measurement of the ratio of inclusive jet cross sections using the anti-kt algorithm with radius parameters R = 0.5 and 0.7 in pp collisions at sqrt(s) = 7 TeV"

description: Inclusive Jet cross section with R = 0.5 in the rapidity bin 0.5 &lt; |y| &lt; 1. The total uncorrelated uncertainty includes statistical one and systematic uncorrelated. The total systematic uncertainty includes all other sources, especially the luminosity uncertainty of 2.2%. The total error can be obtained as a quadratic sum of uncorrelated and correlated one. The NP correction can be used to scale theory prediction to compare to data at particle level.
description: CERN-LHC. Measurements of the inclusive jet cross section with the anti-kt clustering algorithm are presented for two radius parameters, R=0.5 and 0.7. They are based on data from LHC proton-proton collisions at $\sqrt{s}$ = 7 TeV corresponding to an integrated luminosity of 5.0 inverse femtobarns collected with the CMS detector in 2011. The ratio of these two measurements is obtained as a function of the rapidity and transverse momentum of the jets. Significant discrepancies are found comparing the data to leading-order simulations and to fixed-order calculations at next-to-leading order, corrected for nonperturbative effects, whereas simulations with next-to-leading-order matrix elements matched to parton showers describe the data best.
DOI: 10.17182/hepdata.68020.v1/t3
title: "Table 3" of "Measurement of the ratio of inclusive jet cross sections using the anti-kt algorithm with radius parameters R = 0.5 and 0.7 in pp collisions at sqrt(s) = 7 TeV"

description: Inclusive Jet cross section with R = 0.5 in the rapidity bin 1 &lt; |y| &lt; 1.5. The total uncorrelated uncertainty includes statistical one and systematic uncorrelated. The total systematic uncertainty includes all other sources, especially the luminosity uncertainty of 2.2%. The total error can be obtained as a quadratic sum of uncorrelated and correlated one. The NP correction can be used to scale theory prediction to compare to data at particle level.
description: CERN-LHC. Measurements of the inclusive jet cross section with the anti-kt clustering algorithm are presented for two radius parameters, R=0.5 and 0.7. They are based on data from LHC proton-proton collisions at $\sqrt{s}$ = 7 TeV corresponding to an integrated luminosity of 5.0 inverse femtobarns collected with the CMS detector in 2011. The ratio of these two measurements is obtained as a function of the rapidity and transverse momentum of the jets. Significant discrepancies are found comparing the data to leading-order simulations and to fixed-order calculations at next-to-leading order, corrected for nonperturbative effects, whereas simulations with next-to-leading-order matrix elements matched to parton showers describe the data best.
DOI: 10.17182/hepdata.68020.v1/t10
title: "Table 10" of "Measurement of the ratio of inclusive jet cross sections using the anti-kt algorithm with radius parameters R = 0.5 and 0.7 in pp collisions at sqrt(s) = 7 TeV"

description: Inclusive Jet cross section with R = 0.7 in the rapidity bin 1.5 &lt; |y| &lt; 2. The total uncorrelated uncertainty includes statistical one and systematic uncorrelated. The total systematic uncertainty includes all other sources, especially the luminosity uncertainty of 2.2%. The total error can be obtained as a quadratic sum of uncorrelated and correlated one. The NP correction can be used to scale theory prediction to compare to data at particle level.
description: CERN-LHC. Measurements of the inclusive jet cross section with the anti-kt clustering algorithm are presented for two radius parameters, R=0.5 and 0.7. They are based on data from LHC proton-proton collisions at $\sqrt{s}$ = 7 TeV corresponding to an integrated luminosity of 5.0 inverse femtobarns collected with the CMS detector in 2011. The ratio of these two measurements is obtained as a function of the rapidity and transverse momentum of the jets. Significant discrepancies are found comparing the data to leading-order simulations and to fixed-order calculations at next-to-leading order, corrected for nonperturbative effects, whereas simulations with next-to-leading-order matrix elements matched to parton showers describe the data best.
DOI: 10.17182/hepdata.68020.v1/t4
title: "Table 4" of "Measurement of the ratio of inclusive jet cross sections using the anti-kt algorithm with radius parameters R = 0.5 and 0.7 in pp collisions at sqrt(s) = 7 TeV"

description: Inclusive Jet cross section with R = 0.5 in the rapidity bin 1.5 &lt; |y| &lt; 2. The total uncorrelated uncertainty includes statistical one and systematic uncorrelated. The total systematic uncertainty includes all other sources, especially the luminosity uncertainty of 2.2%. The total error can be obtained as a quadratic sum of uncorrelated and correlated one. The NP correction can be used to scale theory prediction to compare to data at particle level.
description: CERN-LHC. Measurements of the inclusive jet cross section with the anti-kt clustering algorithm are presented for two radius parameters, R=0.5 and 0.7. They are based on data from LHC proton-proton collisions at $\sqrt{s}$ = 7 TeV corresponding to an integrated luminosity of 5.0 inverse femtobarns collected with the CMS detector in 2011. The ratio of these two measurements is obtained as a function of the rapidity and transverse momentum of the jets. Significant discrepancies are found comparing the data to leading-order simulations and to fixed-order calculations at next-to-leading order, corrected for nonperturbative effects, whereas simulations with next-to-leading-order matrix elements matched to parton showers describe the data best.
DOI: 10.17182/hepdata.68020.v1/t5
title: "Table 5" of "Measurement of the ratio of inclusive jet cross sections using the anti-kt algorithm with radius parameters R = 0.5 and 0.7 in pp collisions at sqrt(s) = 7 TeV"

description: Inclusive Jet cross section with R = 0.5 in the rapidity bin 2 &lt; |y| &lt; 2.5. The total uncorrelated uncertainty includes statistical one and systematic uncorrelated. The total systematic uncertainty includes all other sources, especially the luminosity uncertainty of 2.2%. The total error can be obtained as a quadratic sum of uncorrelated and correlated one. The NP correction can be used to scale theory prediction to compare to data at particle level.
description: CERN-LHC. Measurements of the inclusive jet cross section with the anti-kt clustering algorithm are presented for two radius parameters, R=0.5 and 0.7. They are based on data from LHC proton-proton collisions at $\sqrt{s}$ = 7 TeV corresponding to an integrated luminosity of 5.0 inverse femtobarns collected with the CMS detector in 2011. The ratio of these two measurements is obtained as a function of the rapidity and transverse momentum of the jets. Significant discrepancies are found comparing the data to leading-order simulations and to fixed-order calculations at next-to-leading order, corrected for nonperturbative effects, whereas simulations with next-to-leading-order matrix elements matched to parton showers describe the data best.
DOI: 10.17182/hepdata.68020.v1/t6
title: "Table 6" of "Measurement of the ratio of inclusive jet cross sections using the anti-kt algorithm with radius parameters R = 0.5 and 0.7 in pp collisions at sqrt(s) = 7 TeV"

description: Inclusive Jet cross section with R = 0.5 in the rapidity bin 2.5 &lt; |y| &lt; 3. The total uncorrelated uncertainty includes statistical one and systematic uncorrelated. The total systematic uncertainty includes all other sources, especially the luminosity uncertainty of 2.2%. The total error can be obtained as a quadratic sum of uncorrelated and correlated one. The NP correction can be used to scale theory prediction to compare to data at particle level.
description: CERN-LHC. Measurements of the inclusive jet cross section with the anti-kt clustering algorithm are presented for two radius parameters, R=0.5 and 0.7. They are based on data from LHC proton-proton collisions at $\sqrt{s}$ = 7 TeV corresponding to an integrated luminosity of 5.0 inverse femtobarns collected with the CMS detector in 2011. The ratio of these two measurements is obtained as a function of the rapidity and transverse momentum of the jets. Significant discrepancies are found comparing the data to leading-order simulations and to fixed-order calculations at next-to-leading order, corrected for nonperturbative effects, whereas simulations with next-to-leading-order matrix elements matched to parton showers describe the data best.
DOI: 10.17182/hepdata.68020.v1/t7
title: "Table 7" of "Measurement of the ratio of inclusive jet cross sections using the anti-kt algorithm with radius parameters R = 0.5 and 0.7 in pp collisions at sqrt(s) = 7 TeV"

description: Inclusive Jet cross section with R = 0.7 in the rapidity bin 0 &lt; |y| &lt; 0.5. The total uncorrelated uncertainty includes statistical one and systematic uncorrelated. The total systematic uncertainty includes all other sources, especially the luminosity uncertainty of 2.2%. The total error can be obtained as a quadratic sum of uncorrelated and correlated one. The NP correction can be used to scale theory prediction to compare to data at particle level.
description: CERN-LHC. Measurements of the inclusive jet cross section with the anti-kt clustering algorithm are presented for two radius parameters, R=0.5 and 0.7. They are based on data from LHC proton-proton collisions at $\sqrt{s}$ = 7 TeV corresponding to an integrated luminosity of 5.0 inverse femtobarns collected with the CMS detector in 2011. The ratio of these two measurements is obtained as a function of the rapidity and transverse momentum of the jets. Significant discrepancies are found comparing the data to leading-order simulations and to fixed-order calculations at next-to-leading order, corrected for nonperturbative effects, whereas simulations with next-to-leading-order matrix elements matched to parton showers describe the data best.
DOI: 10.17182/hepdata.68020.v1/t8
title: "Table 8" of "Measurement of the ratio of inclusive jet cross sections using the anti-kt algorithm with radius parameters R = 0.5 and 0.7 in pp collisions at sqrt(s) = 7 TeV"

description: Inclusive Jet cross section with R = 0.7 in the rapidity bin 0.5 &lt; |y| &lt; 1. The total uncorrelated uncertainty includes statistical one and systematic uncorrelated. The total systematic uncertainty includes all other sources, especially the luminosity uncertainty of 2.2%. The total error can be obtained as a quadratic sum of uncorrelated and correlated one. The NP correction can be used to scale theory prediction to compare to data at particle level.
description: CERN-LHC. Measurements of the inclusive jet cross section with the anti-kt clustering algorithm are presented for two radius parameters, R=0.5 and 0.7. They are based on data from LHC proton-proton collisions at $\sqrt{s}$ = 7 TeV corresponding to an integrated luminosity of 5.0 inverse femtobarns collected with the CMS detector in 2011. The ratio of these two measurements is obtained as a function of the rapidity and transverse momentum of the jets. Significant discrepancies are found comparing the data to leading-order simulations and to fixed-order calculations at next-to-leading order, corrected for nonperturbative effects, whereas simulations with next-to-leading-order matrix elements matched to parton showers describe the data best.
DOI: 10.17182/hepdata.68020.v1/t9
title: "Table 9" of "Measurement of the ratio of inclusive jet cross sections using the anti-kt algorithm with radius parameters R = 0.5 and 0.7 in pp collisions at sqrt(s) = 7 TeV"

description: Inclusive Jet cross section with R = 0.7 in the rapidity bin 1 &lt; |y| &lt; 1.5. The total uncorrelated uncertainty includes statistical one and systematic uncorrelated. The total systematic uncertainty includes all other sources, especially the luminosity uncertainty of 2.2%. The total error can be obtained as a quadratic sum of uncorrelated and correlated one. The NP correction can be used to scale theory prediction to compare to data at particle level.
description: CERN-LHC. Measurements of the inclusive jet cross section with the anti-kt clustering algorithm are presented for two radius parameters, R=0.5 and 0.7. They are based on data from LHC proton-proton collisions at $\sqrt{s}$ = 7 TeV corresponding to an integrated luminosity of 5.0 inverse femtobarns collected with the CMS detector in 2011. The ratio of these two measurements is obtained as a function of the rapidity and transverse momentum of the jets. Significant discrepancies are found comparing the data to leading-order simulations and to fixed-order calculations at next-to-leading order, corrected for nonperturbative effects, whereas simulations with next-to-leading-order matrix elements matched to parton showers describe the data best.
DOI: 10.17182/hepdata.68020.v1/t11
title: "Table 11" of "Measurement of the ratio of inclusive jet cross sections using the anti-kt algorithm with radius parameters R = 0.5 and 0.7 in pp collisions at sqrt(s) = 7 TeV"

description: Inclusive Jet cross section with R = 0.7 in the rapidity bin 2 &lt; |y| &lt; 2.5. The total uncorrelated uncertainty includes statistical one and systematic uncorrelated. The total systematic uncertainty includes all other sources, especially the luminosity uncertainty of 2.2%. The total error can be obtained as a quadratic sum of uncorrelated and correlated one. The NP correction can be used to scale theory prediction to compare to data at particle level.
description: CERN-LHC. Measurements of the inclusive jet cross section with the anti-kt clustering algorithm are presented for two radius parameters, R=0.5 and 0.7. They are based on data from LHC proton-proton collisions at $\sqrt{s}$ = 7 TeV corresponding to an integrated luminosity of 5.0 inverse femtobarns collected with the CMS detector in 2011. The ratio of these two measurements is obtained as a function of the rapidity and transverse momentum of the jets. Significant discrepancies are found comparing the data to leading-order simulations and to fixed-order calculations at next-to-leading order, corrected for nonperturbative effects, whereas simulations with next-to-leading-order matrix elements matched to parton showers describe the data best.
DOI: 10.17182/hepdata.68020.v1/t12
title: "Table 12" of "Measurement of the ratio of inclusive jet cross sections using the anti-kt algorithm with radius parameters R = 0.5 and 0.7 in pp collisions at sqrt(s) = 7 TeV"

description: Inclusive Jet cross section with R = 0.7 in the rapidity bin 2.5 &lt; |y| &lt; 3. The total uncorrelated uncertainty includes statistical one and systematic uncorrelated. The total systematic uncertainty includes all other sources, especially the luminosity uncertainty of 2.2%. The total error can be obtained as a quadratic sum of uncorrelated and correlated one. The NP correction can be used to scale theory prediction to compare to data at particle level.
description: CERN-LHC. Measurements of the inclusive jet cross section with the anti-kt clustering algorithm are presented for two radius parameters, R=0.5 and 0.7. They are based on data from LHC proton-proton collisions at $\sqrt{s}$ = 7 TeV corresponding to an integrated luminosity of 5.0 inverse femtobarns collected with the CMS detector in 2011. The ratio of these two measurements is obtained as a function of the rapidity and transverse momentum of the jets. Significant discrepancies are found comparing the data to leading-order simulations and to fixed-order calculations at next-to-leading order, corrected for nonperturbative effects, whereas simulations with next-to-leading-order matrix elements matched to parton showers describe the data best.