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 6 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.

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 6 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.

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 6 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.

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 6 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.

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 6 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.

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 7 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.

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.

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.

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.

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.

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.

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.

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.

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.

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.

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.

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.

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.

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.

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.

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.

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.

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.

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.

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.

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.

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.

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.

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.

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.

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.

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.

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.

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.

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.

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.

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.

Normalised 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 11 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.

Normalised 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 11 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.

Normalised 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 11 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.

Normalised 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 11 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.

Normalised 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 11 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.

Normalised 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 11 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.

Normalised 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 11 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.

Normalised 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 11 of the paper (arXiv:1611.03421v3) should be swapped. See Table 5 of arXiv:1406.4709v2 for details of the correlation model.

Matrix of statistical correlation coefficients of the unfolded jet cross sections at low $Q^2$.

Matrix of statistical correlation coefficients of the unfolded normalised jet cross sections at low $Q^2$.

Inclusive jet cross sections for $P_T^{\rm jet}$ = 5-7 GeV$^2$ measured as a function of $Q^2$ in the range 150-15000 GeV$^2$. The cross section values and uncertainties have been determined in the scope of the analysis of an earlier H1 publication (<a href="https://inspirehep.net/record/1301218">INSPIRE</a>, <a href="https://www.hepdata.net/record/ins1301218">HEPData</a>). See Table 5 of arXiv:1406.4709v2 for details of the correlation model.

Normalised inclusive jet cross sections for $P_T^{\rm jet}$ = 5-7 GeV$^2$ measured as a function of $Q^2$ in the range 150-15000 GeV$^2$. The cross section values and uncertainties have been determined in the scope of the analysis of an earlier H1 publication (<a href="https://inspirehep.net/record/1301218">INSPIRE</a>, <a href="https://www.hepdata.net/record/ins1301218">HEPData</a>). See Table 5 of arXiv:1406.4709v2 for details of the correlation model.

Matrix of statistical correlation coefficients of the unfolded jet cross sections at high $Q^2$. The statistical correlations have been determined in the scope of the analysis of an earlier H1 publication (<a href="https://inspirehep.net/record/1301218">INSPIRE</a>, <a href="https://www.hepdata.net/record/ins1301218">HEPData</a>).

Matrix of statistical correlation coefficients of the unfolded normalised jet cross sections at high $Q^2$. The statistical correlations have been determined in the scope of the analysis of an earlier H1 publication (<a href="https://inspirehep.net/record/1301218">INSPIRE</a>, <a href="https://www.hepdata.net/record/ins1301218">HEPData</a>).

The strong coupling extracted from the normalised inclusive jet, dijet and trijet data at NLO as a function of the renormalisation scale $\mu_r$. For each $\mu_r$ the values of the strong coupling $\alpha_s(\mu_r)$ and the equivalent values $\alpha_s(M_Z)$ are given with experimental (exp) and theoretical (th) uncertainties.

Unfolded $\nu_\mu$ CC1$\pi^+$ differential cross section as a function of $p_\mu$ in the reduced phase-space of $p_{\pi^+} > 200$ MeV/$c$, $p_\mu > 200$ MeV/c, $\cos(\theta_{\pi^+}) > 0.3$ and $\cos(\theta_\mu) > 0.3$.

Unfolded $\nu_\mu$ CC1$\pi^+$ differential cross section as a function of $\cos\theta_\mu$ in the reduced phase-space of $p_{\pi^+} > 200$ MeV/$c$, $p_\mu > 200$ MeV/c, $\cos(\theta_{\pi^+}) > 0.3$ and $\cos(\theta_\mu) > 0.3$.

Unfolded $\nu_\mu$ CC1$\pi^+$ differential cross section as a function of $\cos\theta_{\mu,\pi}$ in the reduced phase-space of $p_{\pi^+} > 200$ MeV/$c$, $p_\mu > 200$ MeV/c, $\cos(\theta_{\pi^+}) > 0.3$ and $\cos(\theta_\mu) > 0.3$.

Unfolded $\nu_\mu$ CC1$\pi^+$ differential cross section as a function of $E_\nu^{\rm rec}$ ($\Delta$) in the reduced phase-space of $p_{\pi^+} > 200$ MeV/$c$, $p_\mu > 200$ MeV/c, $\cos(\theta_{\pi^+}) > 0.3$ and $\cos(\theta_\mu) > 0.3$.

Unfolded $\nu_\mu$ CC1$\pi^+$ differential cross section as a function of $E_\nu^{\rm rec}$ ($\mu$, $\pi$) in the reduced phase-space of $p_{\pi^+} > 200$ MeV/$c$, $p_\mu > 200$ MeV/c, $\cos(\theta_{\pi^+}) > 0.3$ and $\cos(\theta_\mu) > 0.3$.

1$\sigma$ C.L. contour in $\sin^{2}\bar{\theta}_{23}$-$\Delta\bar{m}^{2}_{32}$ plane (inverted hierarchy).

90% C.L. contour in $\sin^{2}\bar{\theta}_{23}$-$\Delta\bar{m}^{2}_{32}$ plane (inverted hierarchy).

Best-fit point in $\sin^{2}\bar{\theta}_{23}$-$\Delta\bar{m}^{2}_{32}$ plane (inverted hierarchy).

Multiplicity distributions measured in the current region of the Breit frame for the bin of 2*E(Breit,current region) = 12 to 20.

Multiplicity distributions measured in the current region of the Breit frame for the bin of 2*E(Breit,current region) = 20 to 30.

Multiplicity distributions measured in the current region of the Breit frame for the bin of 2*E(Breit,current region) = 30 to 45.

Multiplicity distributions measured in the current region of the Breit frame for the bin of 2*E(Breit,current region) = 45 to 100.

Multiplicity distributions measured in the current region of the Breit frame for the Meff bin 1.5 to 4.

Multiplicity distributions measured in the current region of the Breit frame for the Meff bin 4 to 8.

Multiplicity distributions measured in the current region of the Breit frame for the Meff bin 8 to 12.

Multiplicity distributions measured in the current region of the Breit frame for the Meff bin 12 to 20.

Multiplicity distributions measured in the current region of the hadronic centre of mass (HCM) frame for W = 70 to 100 GeV.

Multiplicity distributions measured in the current region of the hadronic centre of mass (HCM) frame for W = 100 to 150 GeV.

Multiplicity distributions measured in the current region of the hadronic centre of mass (HCM) frame for W = 150 to 225 GeV.

Multiplicity distributions measured in the current region of the hadronic centre of mass (HCM) frame for the Meff bin 1.5 to 4.

Multiplicity distributions measured in the current region of the hadronic centre of mass (HCM) frame for the Meff bin 4 to 8.

Multiplicity distributions measured in the current region of the hadronic centre of mass (HCM) frame for the Meff bin 8 to 12.

Multiplicity distributions measured in the current region of the hadronic centre of mass (HCM) frame for the Meff bin 12 to 20.

Multiplicity distributions measured in the current region of the hadronic centre of mass (HCM) frame for the Meff bin 20 to 30.

Mean charged multiplicity measured in the Breit frame as a function of 2*E(Breit current region) with the assumptions of stable or decaying K0 and LAMBDA particles.

Mean charged multiplicity measured to the current fragmentation region of the HCM frame as a function of W with the assumptions of stable or decaying K0 and LAMBDA particles.

Mean charged multiplicity measured in the Breit frame as a function of Meff with the assumptions of stable or decaying K0 and LAMBDA particles.

Mean charged multiplicity measured in the current fragmentation region of the HCM frame as a function of Meff with the assumptions of stable or decaying K0 and LAMBDA particles.

Differential polarized inclusive jet cross sections as a function of jet transverse energy.

Differential polarized inclusive jet cross sections as a function of photon virtuality, Q**2.

Differential polarized inclusive jet cross sections as a function of photon virtuality, Q**2.

Differential polarized inclusive jet cross sections as a function of X. Update: contrary to the publication, this is D(SIG)/DLOG10(X) not D(SIG)/DX.

Differential polarized inclusive jet cross sections as a function of X. Update: contrary to the publication, this is D(SIG)/DLOG10(X) not D(SIG)/DX.

Integrated polarized inclusive-jet cross section in the given kinematical range for the E- beam.

Integrated polarized inclusive-jet cross section in the given kinematical range for the E+ beam.

Differential unpolarized cross section for single jet production as a function of the jet pseudorapidity.

Differential unpolarized cross section for two jet production as a function of the mean jet pseudorapidity.

Differential unpolarized cross section for three jet production as a function of the mean jet pseudorapidity.

Differential unpolarized cross section for single jet production as a function of the jet transverse energy.

Differential unpolarized cross section for two jet production as a function of the mean jet transverse energy.

Differential unpolarized cross section for three jet production as a function of the mean jet transverse energy.

Differential unpolarized cross section for single jet production as a function of photon virtuality, Q**2.

Differential unpolarized cross section for two jet production as a function of photon virtuality, Q**2.

Differential unpolarized cross section for three jet production as a function of photon virtuality, Q**2.

Differential unpolarized inclusive-jet cross section as a function of X. Update: contrary to the publication, this is D(SIG)/DLOG10(X) not D(SIG)/DX.

Integrated unpolarized jet cross section in the given kinemetical region.

Differential unpolarized dijet cross section as a function of the dijet mass.

Differential unpolarized three-jet cross section as a function of the three-jet mass.

Antineutrino forward dimuon cross sections for Y bins 0.35, 0.58 and 0.78 as a function of X for neutrino energy 78.

Antineutrino forward dimuon cross sections for Y bins 0.35, 0.58 and 0.78 as a function of X for neutrino energy 144.

Antineutrino forward dimuon cross sections for Y bins 0.35, 0.58 and 0.78 as a function of X for neutrino energy 227.

Differential cross section DSIG/DZ(NAME=POMERON) for diffractive photoproduction of dijets as a function of Z(NAME=POMERON).

Differential cross section for the diffractive photoproduction of dijets as a function of ET of the highest jet.

Differential cross section for the diffractive photoproduction of dijets as a function of pseudorapidity (ETARAP) of the highest ET jet.

Differential cross section for the diffractive photoproduction of dijets as a function of X(C=GAMMA,OBS).

Differential cross section DSIG/DY for diffractive photoproduction of dijets as a function of Y for X(C=GAMMA,OBS) > 0.75.

Differential cross section DSIG/DM(P=5_6_7) for diffractive photoproduction of dijets as a function of M(P=5_6_7) for X(C=GAMMA,OBS) > 0.75.

Differential cross section DSIG/DX(NAME=POMERON) for diffractive photoproduction of dijets as a function of X(NAME=POMERON) for X(C=GAMMA,OBS) > 0.75.

Differential cross section DSIG/DZ(NAME=POMERON) for diffractive photoproduction of dijets as a function of Z(NAME=POMERON) for X(C=GAMMA,OBS) > 0.75.

Differential cross section DSIG/DY for diffractive photoproduction of dijets as a function of Y for X(C=GAMMA,OBS) < 0.75.

Differential cross section DSIG/DM(P=5_6_7) for diffractive photoproduction of dijets as a function of M(P=5_6_7) for X(C=GAMMA,OBS) < 0.75.

Differential cross section DSIG/DX(NAME=POMERON) for diffractive photoproduction of dijets as a function of X(NAME=POMERON) for X(C=GAMMA,OBS) < 0.75.

Differential cross section DSIG/DZ(NAME=POMERON) for diffractive photoproduction of dijets as a function of Z(NAME=POMERON) for X(C=GAMMA,OBS) < 0.75.

Measurement of F2 at X = 0.125.

Measurement of F2 at X = 0.175.

Measurement of F2 at X = 0.225.

Measurement of F2 at X = 0.275.

Measurement of F2 at X = 0.350.

Measurement of F2 at X = 0.450.

Measurement of F2 at X = 0.550.

Measurement of F2 at X = 0.650.

Measurement of F2 at X = 0.750.

Measurement of XF3 at X = 0.015.

Measurement of XF3 at X = 0.045.

Measurement of XF3 at X = 0.080.

Measurement of XF3 at X = 0.125.

Measurement of XF3 at X = 0.175.

Measurement of XF3 at X = 0.225.

Measurement of XF3 at X = 0.275.

Measurement of XF3 at X = 0.350.

Measurement of XF3 at X = 0.450.

Measurement of XF3 at X = 0.550.

Measurement of XF3 at X = 0.650.

Measurement of XF3 at X = 0.750.

Differential cross sections at neutrino energy 35.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 35.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 35.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 35.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 45.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 45.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 45.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 45.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 55.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 55.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 55.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 55.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 65.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 65.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 65.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 65.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 75.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 75.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 75.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 75.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 85.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 85.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 85.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 85.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 95.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 95.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 95.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 95.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 110.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 110.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 110.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 110.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 130.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 130.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 130.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 130.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 150.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 150.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 150.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 150.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 170.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 170.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 170.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 170.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 190.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 190.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 190.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 190.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 215.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 215.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 215.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 215.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 245.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 245.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 245.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 245.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 275.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 275.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 275.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 275.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 305.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 305.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 305.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 305.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at neutrino energy 340.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at neutrino energy 340.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at neutrino energy 340.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at neutrino energy 340.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 35.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 35.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 35.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 35.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 45.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 45.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 45.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 45.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 55.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 55.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 55.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 55.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 65.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 65.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 65.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 65.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 75.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 75.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 75.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 75.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 85.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 85.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 85.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 85.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 95.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 95.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 95.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 95.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 110.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 110.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 110.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 110.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 130.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 130.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 130.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 130.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 150.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 150.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 150.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 150.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 170.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 170.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 170.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 170.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 190.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 190.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 190.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 190.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 215.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 215.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 215.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 215.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 245.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 245.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 245.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 245.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 275.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 275.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 275.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 275.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 305.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 305.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 305.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Differential cross sections at antineutrino energy 305.0 GeV as a function of inelasticity Y for X values 0.550, 0.650 and 0.750.

Differential cross sections at antineutrino energy 340.0 GeV as a function of inelasticity Y for X values 0.015, 0.045 and 0.080.

Differential cross sections at antineutrino energy 340.0 GeV as a function of inelasticity Y for X values 0.125, 0.175 and 0.225.

Differential cross sections at antineutrino energy 340.0 GeV as a function of inelasticity Y for X values 0.275, 0.350 and 0.450.

Measured differential cross section as a function of PT.

Measured differential cross section as a function of ETARAP.

Differential cross section as a function of PT for Q**2 from 40 to 1000 GeV**2.

Differential cross section as a function of ETARAP for Q**2 from 40 to 1000GeV**2.

Measured cross section in Q**2, Y bins.

Measured cross section in Q**2, Y bins.

Measured cross section in Q**2, Y bins.

Measured cross section in Q**2, Y bins.

Measured cross section in Q**2, Y bins.

Measured cross section in Q**2, Y bins.

Measured cross section in Q**2, Y bins.

Measured cross section in Q**2, Y bins.

Measured cross section in Q**2, Y bins.

Extracted values of the charm structure function F2(C=CHARM) plus the F2 value from the ZEUS NLO QCD fit. The second DSYS is the theoretical uncertainty.

The differential cross section as a function of Y.

The reduced cross section as a function of Q**2 and X.

The reduced cross section as a function of Q**2 and X.

The reduced cross section as a function of Q**2 and X.

The reduced cross section as a function of Q**2 and X.

The reduced cross section as a function of Q**2 and X.

The reduced cross section as a function of Q**2 and X.

The reduced cross section as a function of Q**2 and X.

The reduced cross section as a function of Q**2 and X.