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).

Asymmetry results on $\vec e-^2$H parity-violating scattering from the PVDIS experiment at JLab, for RES IV settings.

Asymmetry results on $\vec e-^2$H parity-violating scattering from the PVDIS experiment at JLab, for RES III settings.

A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.1900 GeV.

A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.2100 GeV.

A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.2300 GeV.

A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.2500 GeV.

A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.2700 GeV.

A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.2900 GeV.

A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.3100 GeV.

A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.3300 GeV.

A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.3500 GeV.

A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.3700 GeV.

A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.3900 GeV.

A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.4100 GeV.

A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.4300 GeV.

A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.4500 GeV.

A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.4700 GeV.

A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.4900 GeV.

A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.5100 GeV.

A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.5300 GeV.

A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.5500 GeV.

A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.5700 GeV.

A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.5900 GeV.

A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.6100 GeV.

A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.6300 GeV.

A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.6500 GeV.

A1 and g1/F1 for the P target at incident energy 1.6000 GeV and W = 1.1100 GeV.

A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 1.1750 GeV.

A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 1.2250 GeV.

A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 1.2750 GeV.

A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 1.3250 GeV.

A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 1.3750 GeV.

A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 1.4250 GeV.

A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 1.4750 GeV.

A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 1.5250 GeV.

A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 1.5750 GeV.

A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 1.6250 GeV.

A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 1.6750 GeV.

A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 1.7250 GeV.

A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 1.7750 GeV.

A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 1.8250 GeV.

A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 1.8750 GeV.

A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 1.9250 GeV.

A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 1.9750 GeV.

A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 2.0250 GeV.

A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 2.0750 GeV.

A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 2.1250 GeV.

A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 2.1750 GeV.

A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 2.2250 GeV.

A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 2.2750 GeV.

A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 2.3250 GeV.

A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 2.3750 GeV.

A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 2.4250 GeV.

A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 2.4750 GeV.

A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 2.5250 GeV.

A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 2.5750 GeV.

A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 2.6250 GeV.

A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 2.6750 GeV.

A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 2.7250 GeV.

A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 2.7750 GeV.

A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 2.8250 GeV.

A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 2.8750 GeV.

A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 2.9250 GeV.

A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 2.9750 GeV.

A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 3.0250 GeV.

A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 3.0750 GeV.

A1 and g1/F1 for the P target at incident energy 5.7000 GeV and W = 1.1250 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.0850 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.0850 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.0950 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.0950 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.1050 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.1050 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.1150 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.1150 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.1250 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.1250 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.1350 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.1350 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.1450 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.1450 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.1550 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.1550 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.1650 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.1650 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.1750 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.1750 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.1850 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.1850 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.1950 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.1950 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.2050 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.2050 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.2150 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.2150 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.2250 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.2250 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.2350 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.2350 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.2450 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.2450 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.2550 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.2550 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.2650 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.2650 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.2750 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.2750 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.2850 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.2850 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.2950 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.2950 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.3050 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.3050 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.3150 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.3150 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.3250 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.3250 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.3350 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.3350 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.3450 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.3450 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.3550 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.3550 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.3650 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.3650 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.3750 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.3750 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.3850 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.3850 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.3950 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.3950 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.4050 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.4050 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.4150 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.4150 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.4250 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.4250 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.4350 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.4350 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.4450 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.4450 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.4550 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.4550 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.4650 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.4650 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.4750 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.4750 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.4850 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.4850 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.4950 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.4950 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.5050 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.5050 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.5150 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.5150 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.5250 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.5250 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.5350 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.5350 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.5450 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.5450 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.5550 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.5550 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.5650 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.5650 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.5750 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.5750 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.5850 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.5850 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.5950 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.5950 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.6050 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.6050 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.6150 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.6150 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.6250 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.6250 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.6350 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.6350 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.6450 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.6450 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.6550 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.6550 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.6650 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.6650 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.6750 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.6750 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.6850 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.6850 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.6950 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.6950 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.7050 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.7050 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.7150 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.7150 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.7250 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.7250 GeV.

A1 and g1/F1 for the DEUT target at incident energy 1.6000 GeV and W = 1.7350 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.7350 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.7450 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.7550 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.7650 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.7750 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.7850 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.7950 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.8050 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.8150 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.8250 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.8350 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.8450 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.8550 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.8650 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.8750 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.8850 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.8950 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.9050 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.9150 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.9250 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.9350 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.9450 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.9550 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.9650 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.9750 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.9850 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 1.9950 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.0050 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.0150 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.0250 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.0350 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.0450 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.0550 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.0650 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.0750 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.0850 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.0950 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.1050 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.1150 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.1250 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.1350 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.1450 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.1550 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.1650 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.1750 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.1850 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.1950 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.2050 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.2150 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.2250 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.2350 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.2450 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.2550 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.2650 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.2750 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.2850 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.2950 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.3050 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.3150 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.3250 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.3350 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.3450 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.3550 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.3650 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.3750 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.3850 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.3950 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.4050 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.4150 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.4250 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.4350 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.4450 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.4550 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.4650 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.4750 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.4850 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.4950 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.5050 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.5150 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.5250 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.5350 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.5450 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.5550 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.5650 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.5750 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.5850 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.5950 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.6050 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.6150 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.6250 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.6350 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.6450 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.6550 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.6650 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.6750 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.6850 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.6950 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.7050 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.7150 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.7250 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.7350 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.7450 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.7550 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.7650 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.7750 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.7850 GeV.

A1 and g1/F1 for the DEUT target at incident energy 5.7000 GeV and W = 2.7950 GeV.

Triple differential cross section.

Cross sections for di-jet and forward jet data.. The jets are ordered such that:-. ETARAP(P=4) > ETARAP(P=5) > ETARAP(P=6).. The first jet (P=4) is the forward jet.

Cross sections for di-jet and forward jet data.. The jets are ordered such that:-. ETARAP(P=4) > ETARAP(P=5) > ETARAP(P=6).. The first jet (P=4) is the forward jet.

Cross sections for di-jet and forward jet data.. The jets are ordered such that:-. ETARAP(P=4) > ETARAP(P=5) > ETARAP(P=6).. The first jet (P=4) is the forward jet.