cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.86390.v1/t10
title: "Dijets for $Q^2$ = 8.0-11.0 GeV$^2$" of "Measurement of Jet Production Cross Sections in Deep-inelastic $ep$ Scattering at HERA"

description: Dijet cross sections measured as a function of $\langle P_T \rangle_2$ for $Q^2$ = 8.0-11.0 GeV$^2$. The correction factors on the theoretical cross sections $c^{\rm had}$ are listed together with their uncertainties. The radiative correction factors $c^{\rm rad}$ are already included in the quoted cross sections. Note that the uncertainties labelled $\delta^{E_{e^\prime}}$ and $\delta^{\theta_{e^\prime}}$ in Table 7 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.
description: No data abstract available.
DOI: 10.17182/hepdata.86390.v1/t11
title: "Dijets for $Q^2$ = 11.0-16.0 GeV$^2$" of "Measurement of Jet Production Cross Sections in Deep-inelastic $ep$ Scattering at HERA"

description: Dijet cross sections measured as a function of $\langle P_T \rangle_2$ for $Q^2$ = 11.0-16.0 GeV$^2$. The correction factors on the theoretical cross sections $c^{\rm had}$ are listed together with their uncertainties. The radiative correction factors $c^{\rm rad}$ are already included in the quoted cross sections. Note that the uncertainties labelled $\delta^{E_{e^\prime}}$ and $\delta^{\theta_{e^\prime}}$ in Table 7 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.
description: No data abstract available.
DOI: 10.17182/hepdata.86390.v1/t12
title: "Dijets for $Q^2$ = 16.0-22.0 GeV$^2$" of "Measurement of Jet Production Cross Sections in Deep-inelastic $ep$ Scattering at HERA"

description: Dijet cross sections measured as a function of $\langle P_T \rangle_2$ for $Q^2$ = 16.0-22.0 GeV$^2$. The correction factors on the theoretical cross sections $c^{\rm had}$ are listed together with their uncertainties. The radiative correction factors $c^{\rm rad}$ are already included in the quoted cross sections. Note that the uncertainties labelled $\delta^{E_{e^\prime}}$ and $\delta^{\theta_{e^\prime}}$ in Table 7 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.
description: No data abstract available.
DOI: 10.17182/hepdata.86390.v1/t13
title: "Dijets for $Q^2$ = 22.0-30.0 GeV$^2$" of "Measurement of Jet Production Cross Sections in Deep-inelastic $ep$ Scattering at HERA"

description: Dijet cross sections measured as a function of $\langle P_T \rangle_2$ for $Q^2$ = 22.0-30.0 GeV$^2$. The correction factors on the theoretical cross sections $c^{\rm had}$ are listed together with their uncertainties. The radiative correction factors $c^{\rm rad}$ are already included in the quoted cross sections. Note that the uncertainties labelled $\delta^{E_{e^\prime}}$ and $\delta^{\theta_{e^\prime}}$ in Table 7 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.
description: No data abstract available.
DOI: 10.17182/hepdata.86390.v1/t14
title: "Dijets for $Q^2$ = 30.0-42.0 GeV$^2$" of "Measurement of Jet Production Cross Sections in Deep-inelastic $ep$ Scattering at HERA"

description: Dijet cross sections measured as a function of $\langle P_T \rangle_2$ for $Q^2$ = 30.0-42.0 GeV$^2$. The correction factors on the theoretical cross sections $c^{\rm had}$ are listed together with their uncertainties. The radiative correction factors $c^{\rm rad}$ are already included in the quoted cross sections. Note that the uncertainties labelled $\delta^{E_{e^\prime}}$ and $\delta^{\theta_{e^\prime}}$ in Table 7 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.
description: No data abstract available.
DOI: 10.17182/hepdata.86390.v1/t15
title: "Dijets for $Q^2$ = 42.0-60.0 GeV$^2$" of "Measurement of Jet Production Cross Sections in Deep-inelastic $ep$ Scattering at HERA"

description: Dijet cross sections measured as a function of $\langle P_T \rangle_2$ for $Q^2$ = 42.0-60.0 GeV$^2$. The correction factors on the theoretical cross sections $c^{\rm had}$ are listed together with their uncertainties. The radiative correction factors $c^{\rm rad}$ are already included in the quoted cross sections. Note that the uncertainties labelled $\delta^{E_{e^\prime}}$ and $\delta^{\theta_{e^\prime}}$ in Table 7 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.
description: No data abstract available.
DOI: 10.17182/hepdata.86390.v1/t16
title: "Dijets for $Q^2$ = 60.0-80.0 GeV$^2$" of "Measurement of Jet Production Cross Sections in Deep-inelastic $ep$ Scattering at HERA"

description: Dijet cross sections measured as a function of $\langle P_T \rangle_2$ for $Q^2$ = 60.0-80.0 GeV$^2$. The correction factors on the theoretical cross sections $c^{\rm had}$ are listed together with their uncertainties. The radiative correction factors $c^{\rm rad}$ are already included in the quoted cross sections. Note that the uncertainties labelled $\delta^{E_{e^\prime}}$ and $\delta^{\theta_{e^\prime}}$ in Table 7 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.
description: No data abstract available.
DOI: 10.17182/hepdata.86390.v1/t17
title: "Trijets for $Q^2$ = 5.5-8.0 GeV$^2$" of "Measurement of Jet Production Cross Sections in Deep-inelastic $ep$ Scattering at HERA"

description: Trijet cross sections measured as a function of $\langle P_T \rangle_3$ for $Q^2$ = 5.5-8.0 GeV$^2$. The correction factors on the theoretical cross sections $c^{\rm had}$ are listed together with their uncertainties. The radiative correction factors $c^{\rm rad}$ are already included in the quoted cross sections. Note that the uncertainties labelled $\delta^{E_{e^\prime}}$ and $\delta^{\theta_{e^\prime}}$ in Table 8 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.
description: No data abstract available.
DOI: 10.17182/hepdata.86390.v1/t18
title: "Trijets for $Q^2$ = 8.0-11.0 GeV$^2$" of "Measurement of Jet Production Cross Sections in Deep-inelastic $ep$ Scattering at HERA"

description: Trijet cross sections measured as a function of $\langle P_T \rangle_3$ for $Q^2$ = 8.0-11.0 GeV$^2$. The correction factors on the theoretical cross sections $c^{\rm had}$ are listed together with their uncertainties. The radiative correction factors $c^{\rm rad}$ are already included in the quoted cross sections. Note that the uncertainties labelled $\delta^{E_{e^\prime}}$ and $\delta^{\theta_{e^\prime}}$ in Table 8 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.
description: No data abstract available.
DOI: 10.17182/hepdata.86390.v1/t19
title: "Trijets for $Q^2$ = 11.0-16.0 GeV$^2$" of "Measurement of Jet Production Cross Sections in Deep-inelastic $ep$ Scattering at HERA"

description: Trijet cross sections measured as a function of $\langle P_T \rangle_3$ for $Q^2$ = 11.0-16.0 GeV$^2$. The correction factors on the theoretical cross sections $c^{\rm had}$ are listed together with their uncertainties. The radiative correction factors $c^{\rm rad}$ are already included in the quoted cross sections. Note that the uncertainties labelled $\delta^{E_{e^\prime}}$ and $\delta^{\theta_{e^\prime}}$ in Table 8 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.
description: No data abstract available.
DOI: 10.17182/hepdata.86390.v1/t20
title: "Trijets for $Q^2$ = 16.0-22.0 GeV$^2$" of "Measurement of Jet Production Cross Sections in Deep-inelastic $ep$ Scattering at HERA"

description: Trijet cross sections measured as a function of $\langle P_T \rangle_3$ for $Q^2$ = 16.0-22.0 GeV$^2$. The correction factors on the theoretical cross sections $c^{\rm had}$ are listed together with their uncertainties. The radiative correction factors $c^{\rm rad}$ are already included in the quoted cross sections. Note that the uncertainties labelled $\delta^{E_{e^\prime}}$ and $\delta^{\theta_{e^\prime}}$ in Table 8 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.
description: No data abstract available.
DOI: 10.17182/hepdata.86390.v1/t21
title: "Trijets for $Q^2$ = 22.0-30.0 GeV$^2$" of "Measurement of Jet Production Cross Sections in Deep-inelastic $ep$ Scattering at HERA"

description: Trijet cross sections measured as a function of $\langle P_T \rangle_3$ for $Q^2$ = 22.0-30.0 GeV$^2$. The correction factors on the theoretical cross sections $c^{\rm had}$ are listed together with their uncertainties. The radiative correction factors $c^{\rm rad}$ are already included in the quoted cross sections. Note that the uncertainties labelled $\delta^{E_{e^\prime}}$ and $\delta^{\theta_{e^\prime}}$ in Table 8 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.
description: No data abstract available.
DOI: 10.17182/hepdata.86390.v1/t22
title: "Trijets for $Q^2$ = 30.0-42.0 GeV$^2$" of "Measurement of Jet Production Cross Sections in Deep-inelastic $ep$ Scattering at HERA"

description: Trijet cross sections measured as a function of $\langle P_T \rangle_3$ for $Q^2$ = 30.0-42.0 GeV$^2$. The correction factors on the theoretical cross sections $c^{\rm had}$ are listed together with their uncertainties. The radiative correction factors $c^{\rm rad}$ are already included in the quoted cross sections. Note that the uncertainties labelled $\delta^{E_{e^\prime}}$ and $\delta^{\theta_{e^\prime}}$ in Table 8 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.
description: No data abstract available.
DOI: 10.17182/hepdata.86390.v1/t23
title: "Trijets for $Q^2$ = 42.0-60.0 GeV$^2$" of "Measurement of Jet Production Cross Sections in Deep-inelastic $ep$ Scattering at HERA"

description: Trijet cross sections measured as a function of $\langle P_T \rangle_3$ for $Q^2$ = 42.0-60.0 GeV$^2$. The correction factors on the theoretical cross sections $c^{\rm had}$ are listed together with their uncertainties. The radiative correction factors $c^{\rm rad}$ are already included in the quoted cross sections. Note that the uncertainties labelled $\delta^{E_{e^\prime}}$ and $\delta^{\theta_{e^\prime}}$ in Table 8 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.
description: No data abstract available.
DOI: 10.17182/hepdata.86390.v1/t24
title: "Trijets for $Q^2$ = 60.0-80.0 GeV$^2$" of "Measurement of Jet Production Cross Sections in Deep-inelastic $ep$ Scattering at HERA"

description: Trijet cross sections measured as a function of $\langle P_T \rangle_3$ for $Q^2$ = 60.0-80.0 GeV$^2$. The correction factors on the theoretical cross sections $c^{\rm had}$ are listed together with their uncertainties. The radiative correction factors $c^{\rm rad}$ are already included in the quoted cross sections. Note that the uncertainties labelled $\delta^{E_{e^\prime}}$ and $\delta^{\theta_{e^\prime}}$ in Table 8 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.
description: No data abstract available.
DOI: 10.17182/hepdata.86390.v1/t25
title: "Normalised inclusive jets for $Q^2$ = 5.5-8.0 GeV$^2$" of "Measurement of Jet Production Cross Sections in Deep-inelastic $ep$ Scattering at HERA"

description: Normalised inclusive jet cross sections measured as a function of $P_T^{\rm jet}$ for $Q^2$ = 5.5-8.0 GeV$^2$. The correction factors on the theoretical cross sections $c^{\rm had}$ are listed together with their uncertainties. The radiative correction factors $c^{\rm rad}$ are already included in the quoted cross sections. Note that the uncertainties labelled $\delta^{E_{e^\prime}}$ and $\delta^{\theta_{e^\prime}}$ in Table 9 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.
description: No data abstract available.
DOI: 10.17182/hepdata.86390.v1/t26
title: "Normalised inclusive jets for $Q^2$ = 8.0-11.0 GeV$^2$" of "Measurement of Jet Production Cross Sections in Deep-inelastic $ep$ Scattering at HERA"

description: Normalised inclusive jet cross sections measured as a function of $P_T^{\rm jet}$ for $Q^2$ = 8.0-11.0 GeV$^2$. The correction factors on the theoretical cross sections $c^{\rm had}$ are listed together with their uncertainties. The radiative correction factors $c^{\rm rad}$ are already included in the quoted cross sections. Note that the uncertainties labelled $\delta^{E_{e^\prime}}$ and $\delta^{\theta_{e^\prime}}$ in Table 9 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.
description: No data abstract available.
DOI: 10.17182/hepdata.86390.v1/t27
title: "Normalised inclusive jets for $Q^2$ = 11.0-16.0 GeV$^2$" of "Measurement of Jet Production Cross Sections in Deep-inelastic $ep$ Scattering at HERA"

description: Normalised inclusive jet cross sections measured as a function of $P_T^{\rm jet}$ for $Q^2$ = 11.0-16.0 GeV$^2$. The correction factors on the theoretical cross sections $c^{\rm had}$ are listed together with their uncertainties. The radiative correction factors $c^{\rm rad}$ are already included in the quoted cross sections. Note that the uncertainties labelled $\delta^{E_{e^\prime}}$ and $\delta^{\theta_{e^\prime}}$ in Table 9 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.
description: No data abstract available.
DOI: 10.17182/hepdata.86390.v1/t28
title: "Normalised inclusive jets for $Q^2$ = 16.0-22.0 GeV$^2$" of "Measurement of Jet Production Cross Sections in Deep-inelastic $ep$ Scattering at HERA"

description: Normalised inclusive jet cross sections measured as a function of $P_T^{\rm jet}$ for $Q^2$ = 16.0-22.0 GeV$^2$. The correction factors on the theoretical cross sections $c^{\rm had}$ are listed together with their uncertainties. The radiative correction factors $c^{\rm rad}$ are already included in the quoted cross sections. Note that the uncertainties labelled $\delta^{E_{e^\prime}}$ and $\delta^{\theta_{e^\prime}}$ in Table 9 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.
description: No data abstract available.
DOI: 10.17182/hepdata.86390.v1/t29
title: "Normalised inclusive jets for $Q^2$ = 22.0-30.0 GeV$^2$" of "Measurement of Jet Production Cross Sections in Deep-inelastic $ep$ Scattering at HERA"

description: Normalised inclusive jet cross sections measured as a function of $P_T^{\rm jet}$ for $Q^2$ = 22.0-30.0 GeV$^2$. The correction factors on the theoretical cross sections $c^{\rm had}$ are listed together with their uncertainties. The radiative correction factors $c^{\rm rad}$ are already included in the quoted cross sections. Note that the uncertainties labelled $\delta^{E_{e^\prime}}$ and $\delta^{\theta_{e^\prime}}$ in Table 9 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.
description: No data abstract available.
DOI: 10.17182/hepdata.86390.v1/t30
title: "Normalised inclusive jets for $Q^2$ = 30.0-42.0 GeV$^2$" of "Measurement of Jet Production Cross Sections in Deep-inelastic $ep$ Scattering at HERA"

description: Normalised inclusive jet cross sections measured as a function of $P_T^{\rm jet}$ for $Q^2$ = 30.0-42.0 GeV$^2$. The correction factors on the theoretical cross sections $c^{\rm had}$ are listed together with their uncertainties. The radiative correction factors $c^{\rm rad}$ are already included in the quoted cross sections. Note that the uncertainties labelled $\delta^{E_{e^\prime}}$ and $\delta^{\theta_{e^\prime}}$ in Table 9 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.
description: No data abstract available.
DOI: 10.17182/hepdata.86390.v1/t31
title: "Normalised inclusive jets for $Q^2$ = 42.0-60.0 GeV$^2$" of "Measurement of Jet Production Cross Sections in Deep-inelastic $ep$ Scattering at HERA"

description: Normalised inclusive jet cross sections measured as a function of $P_T^{\rm jet}$ for $Q^2$ = 42.0-60.0 GeV$^2$. The correction factors on the theoretical cross sections $c^{\rm had}$ are listed together with their uncertainties. The radiative correction factors $c^{\rm rad}$ are already included in the quoted cross sections. Note that the uncertainties labelled $\delta^{E_{e^\prime}}$ and $\delta^{\theta_{e^\prime}}$ in Table 9 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.
description: No data abstract available.
DOI: 10.17182/hepdata.86390.v1/t32
title: "Normalised inclusive jets for $Q^2$ = 60.0-80.0 GeV$^2$" of "Measurement of Jet Production Cross Sections in Deep-inelastic $ep$ Scattering at HERA"

description: Normalised inclusive jet cross sections measured as a function of $P_T^{\rm jet}$ for $Q^2$ = 60.0-80.0 GeV$^2$. The correction factors on the theoretical cross sections $c^{\rm had}$ are listed together with their uncertainties. The radiative correction factors $c^{\rm rad}$ are already included in the quoted cross sections. Note that the uncertainties labelled $\delta^{E_{e^\prime}}$ and $\delta^{\theta_{e^\prime}}$ in Table 9 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.
description: No data abstract available.
DOI: 10.17182/hepdata.86390.v1/t33
title: "Normalised dijets for $Q^2$ = 5.5-8.0 GeV$^2$" of "Measurement of Jet Production Cross Sections in Deep-inelastic $ep$ Scattering at HERA"

description: Normalised dijet cross sections measured as a function of $\langle P_T \rangle_2$ for $Q^2$ = 5.5-8.0 GeV$^2$. The correction factors on the theoretical cross sections $c^{\rm had}$ are listed together with their uncertainties. The radiative correction factors $c^{\rm rad}$ are already included in the quoted cross sections. Note that the uncertainties labelled $\delta^{E_{e^\prime}}$ and $\delta^{\theta_{e^\prime}}$ in Table 10 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.
description: No data abstract available.
DOI: 10.17182/hepdata.86390.v1/t34
title: "Normalised dijets for $Q^2$ = 8.0-11.0 GeV$^2$" of "Measurement of Jet Production Cross Sections in Deep-inelastic $ep$ Scattering at HERA"

description: Normalised dijet cross sections measured as a function of $\langle P_T \rangle_2$ for $Q^2$ = 8.0-11.0 GeV$^2$. The correction factors on the theoretical cross sections $c^{\rm had}$ are listed together with their uncertainties. The radiative correction factors $c^{\rm rad}$ are already included in the quoted cross sections. Note that the uncertainties labelled $\delta^{E_{e^\prime}}$ and $\delta^{\theta_{e^\prime}}$ in Table 10 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.
description: No data abstract available.
DOI: 10.17182/hepdata.86390.v1/t35
title: "Normalised dijets for $Q^2$ = 11.0-16.0 GeV$^2$" of "Measurement of Jet Production Cross Sections in Deep-inelastic $ep$ Scattering at HERA"

description: Normalised dijet cross sections measured as a function of $\langle P_T \rangle_2$ for $Q^2$ = 11.0-16.0 GeV$^2$. The correction factors on the theoretical cross sections $c^{\rm had}$ are listed together with their uncertainties. The radiative correction factors $c^{\rm rad}$ are already included in the quoted cross sections. Note that the uncertainties labelled $\delta^{E_{e^\prime}}$ and $\delta^{\theta_{e^\prime}}$ in Table 10 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.
description: No data abstract available.
DOI: 10.17182/hepdata.86390.v1/t36
title: "Normalised dijets for $Q^2$ = 16.0-22.0 GeV$^2$" of "Measurement of Jet Production Cross Sections in Deep-inelastic $ep$ Scattering at HERA"

description: Normalised dijet cross sections measured as a function of $\langle P_T \rangle_2$ for $Q^2$ = 16.0-22.0 GeV$^2$. The correction factors on the theoretical cross sections $c^{\rm had}$ are listed together with their uncertainties. The radiative correction factors $c^{\rm rad}$ are already included in the quoted cross sections. Note that the uncertainties labelled $\delta^{E_{e^\prime}}$ and $\delta^{\theta_{e^\prime}}$ in Table 10 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.
description: No data abstract available.
DOI: 10.17182/hepdata.86390.v1/t37
title: "Normalised dijets for $Q^2$ = 22.0-30.0 GeV$^2$" of "Measurement of Jet Production Cross Sections in Deep-inelastic $ep$ Scattering at HERA"

description: Normalised dijet cross sections measured as a function of $\langle P_T \rangle_2$ for $Q^2$ = 22.0-30.0 GeV$^2$. The correction factors on the theoretical cross sections $c^{\rm had}$ are listed together with their uncertainties. The radiative correction factors $c^{\rm rad}$ are already included in the quoted cross sections. Note that the uncertainties labelled $\delta^{E_{e^\prime}}$ and $\delta^{\theta_{e^\prime}}$ in Table 10 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.
description: No data abstract available.
DOI: 10.17182/hepdata.86390.v1/t38
title: "Normalised dijets for $Q^2$ = 30.0-42.0 GeV$^2$" of "Measurement of Jet Production Cross Sections in Deep-inelastic $ep$ Scattering at HERA"

description: Normalised dijet cross sections measured as a function of $\langle P_T \rangle_2$ for $Q^2$ = 30.0-42.0 GeV$^2$. The correction factors on the theoretical cross sections $c^{\rm had}$ are listed together with their uncertainties. The radiative correction factors $c^{\rm rad}$ are already included in the quoted cross sections. Note that the uncertainties labelled $\delta^{E_{e^\prime}}$ and $\delta^{\theta_{e^\prime}}$ in Table 10 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.
description: No data abstract available.
DOI: 10.17182/hepdata.86390.v1/t39
title: "Normalised dijets for $Q^2$ = 42.0-60.0 GeV$^2$" of "Measurement of Jet Production Cross Sections in Deep-inelastic $ep$ Scattering at HERA"

description: Normalised dijet cross sections measured as a function of $\langle P_T \rangle_2$ for $Q^2$ = 42.0-60.0 GeV$^2$. The correction factors on the theoretical cross sections $c^{\rm had}$ are listed together with their uncertainties. The radiative correction factors $c^{\rm rad}$ are already included in the quoted cross sections. Note that the uncertainties labelled $\delta^{E_{e^\prime}}$ and $\delta^{\theta_{e^\prime}}$ in Table 10 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.
description: No data abstract available.
DOI: 10.17182/hepdata.86390.v1/t40
title: "Normalised dijets for $Q^2$ = 60.0-80.0 GeV$^2$" of "Measurement of Jet Production Cross Sections in Deep-inelastic $ep$ Scattering at HERA"

description: Normalised dijet cross sections measured as a function of $\langle P_T \rangle_2$ for $Q^2$ = 60.0-80.0 GeV$^2$. The correction factors on the theoretical cross sections $c^{\rm had}$ are listed together with their uncertainties. The radiative correction factors $c^{\rm rad}$ are already included in the quoted cross sections. Note that the uncertainties labelled $\delta^{E_{e^\prime}}$ and $\delta^{\theta_{e^\prime}}$ in Table 10 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.
description: No data abstract available.