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D(N)/D(PT**2) HAS BEEN FITTED WITH THE FORMULA A*EXP(-SLOPE(C=1)*PT**2)+C*EXP(-SLOPE(C=2)PT**2).

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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.

Transverse mass spectra for kaon production in the central rapidity region for collisions at 20 GeV per nucleon.

Transverse mass spectra for kaon production in the central rapidity region for collisions at 30 GeV per nucleon.

Rapidity distribution of PI- production.

Rapidity distribution of K- production.

Rapidity distribution of K+ production.

Energy dependence of the mean K+ to PI+ and K- to PI- multiplicity ratio with the full phase space.. The data below 6 GeV are from the AGS and above 100 GeV from RHIC.

Energy dependence of the mean K+ to PI+ and K- to PI- multiplicity ratio mid rapidity regions.. The data below 6 GeV are from the AGS and above 100 GeV from RHIC.

Energy dependence of the inverse slope parameter of the transverse mass spectra in K+ and K- production.. The data below 6 GeV are from the AGS and above 100 GeV from RHIC.

Energy dependence of the mean transverse mass measured at mid rapidity in PI+ and PI- production.. The data below 6 GeV are from the AGS and above 100 GeV from RHIC.

Energy dependence of the mean transverse mass measured at mid rapidity in K+ and K- production.. The data below 6 GeV are from the AGS and above 100 GeV from RHIC.

PHI transverse momentum spectra at incident energy 80 GeV/nucleon integrated over the rapidity range 0 to 1.7.

PHI transverse momentum spectra at incident energy 158 GeV/nucleon integrated over the rapidity range 0 to 1.0.

PHI transverse mass spectra at incident energy 20 GeV/nucleon integrated over the rapidity range 0 to 1.8.

PHI transverse mass spectra at incident energy 30 GeV/nucleon integrated over the rapidity range 0 to 1.8.

PHI transverse mass spectra at incident energy 40 GeV/nucleon integrated over the rapidity range 0 to 1.5.

PHI transverse mass spectra at incident energy 80 GeV/nucleon integrated over the rapidity range 0 to 1.7.

PHI transverse mass spectra at incident energy 158 GeV/nucleon integrated over the rapidity range 0 to 1.0.

Slope parameter as a function of rapidity for incident energy 158 GeV/nucleon. Here slope is defined as :-. DN/DPT = CONST*PT*EXP(-MT/SLOPE).

PHI rapidity distributions for incident energy 20 GeV/nucleon.

PHI rapidity distributions for incident energy 30 GeV/nucleon.

PHI rapidity distributions for incident energy 40 GeV/nucleon.

PHI rapidity distributions for incident energy 80 GeV/nucleon.

PHI rapidity distributions for incident energy 158 GeV/nucleon.

PHI/PI ratio extrapolated to final phase space.

PHI/PI ratio at mid rapidity.

PHI multiplicity.

Values of slope parameter, mean PT and mean MT as a function of energy.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

PT integrated invariant cross sections and density distributions together with mean values of PT and PT**2 as a function of Feynman X for positive pion production.

PT integrated invariant cross sections and density distributions together with mean values of PT and PT**2 as a function of Feynman X for negative pion production.

PT integrated rapidity distribution.

Numerical data for the transverse momentum spectra of helium-3 in rapidity interval

Numerical data for the transverse momentum spectra of helium-3 in rapidity interval

Numerical data for the transverse momentum spectra of helium-3 in rapidity interval

Numerical data for the transverse momentum spectra of helium-3 in rapidity interval

Numerical data for the transverse momentum spectra of helium-3 in rapidity interval

Numerical data for the transverse momentum spectra of helium-3 in rapidity interval

Numerical data for the transverse momentum spectra of helium-3 in rapidity interval

Numerical data for the transverse momentum spectra of helium-3 in rapidity interval

Numerical data for the transverse momentum spectra of helium-3 in rapidity interval

Numerical data for the transverse momentum spectra of helium-3 in rapidity interval

Numerical data for the transverse momentum spectra of helium-3 in rapidity interval

Numerical data for the transverse momentum spectra of helium-3 in rapidity interval

Numerical data for the transverse momentum spectra of helium-3 in rapidity interval

Numerical data for the transverse momentum spectra of helium-3 in rapidity interval

Numerical data for the transverse momentum spectra of helium-3 in rapidity interval

Numerical data for the transverse momentum spectra of helium-3 in rapidity interval

Numerical data for the transverse momentum spectra of helium-3 in rapidity interval

Numerical data for the transverse momentum spectra of helium-3 in rapidity interval

Numerical data for the transverse momentum spectra of helium-3 in rapidity interval

Numerical data for the transverse momentum spectra of helium-3 in rapidity interval

Numerical data for the transverse momentum spectra of helium-3 in rapidity interval

Numerical data for the transverse momentum spectra of helium-3 in rapidity interval

Numerical data for the transverse momentum spectra of helium-3 in rapidity interval

Numerical data for the transverse momentum spectra of helium-3 in rapidity interval

Numerical data for the transverse momentum spectra of helium-3 in rapidity interval

Numerical data for the transverse momentum spectra of helium-3 in rapidity interval

Numerical data for the transverse momentum spectra of helium-3 in rapidity interval

Numerical data for the transverse momentum spectra of helium-3 in rapidity interval

Numerical data for the transverse momentum spectra of helium-3 in rapidity interval

Numerical data for the transverse momentum spectra of helium-3 in rapidity interval

Numerical data for the transverse momentum spectra of helium-3 in rapidity interval

Numerical data for the transverse momentum spectra of helium-3 in rapidity interval

Numerical data for the transverse momentum spectra of helium-3 in rapidity interval

Numerical data for the transverse momentum spectra of helium-3 in rapidity interval

Numerical data for the transverse momentum spectra of helium-3 in rapidity interval

Numerical data for the transverse momentum spectra of helium-3 in rapidity interval

Numerical data for the transverse momentum spectra of helium-3 in rapidity interval

Numerical data for the transverse momentum spectra of deuterons in rapidity interval

Numerical data for the transverse momentum spectra of deuterons in rapidity interval

Numerical data for the transverse momentum spectra of deuterons in rapidity interval

Numerical data for the transverse momentum spectra of deuterons in rapidity interval

Numerical data for the transverse momentum spectra of deuterons in rapidity interval

Numerical data for the transverse momentum spectra of deuterons in rapidity interval

Numerical data for the transverse momentum spectra of deuterons in rapidity interval

Numerical data for the transverse momentum spectra of deuterons in rapidity interval

Numerical data for the transverse momentum spectra of deuterons in rapidity interval

Numerical data for the transverse momentum spectra of deuterons in rapidity interval

Numerical data for the transverse momentum spectra of deuterons in rapidity interval

Numerical data for the transverse momentum spectra of deuterons in rapidity interval

Numerical data for the transverse momentum spectra of deuterons in rapidity interval

Numerical data for the transverse momentum spectra of deuterons in rapidity interval

Numerical data for the transverse momentum spectra of deuterons in rapidity interval

Numerical data for the transverse momentum spectra of tritons in rapidity interval

Numerical data for the transverse momentum spectra of tritons in rapidity interval

Numerical data for the transverse momentum spectra of tritons in rapidity interval

Numerical data for the transverse momentum spectra of tritons in rapidity interval

Numerical data for the transverse momentum spectra of tritons in rapidity interval

Numerical data for the transverse mass spectra of Helium-3 in rapidity interval

Numerical data for the transverse mass spectra of Helium-3 in rapidity interval

Numerical data for the transverse mass spectra of Helium-3 in rapidity interval

Numerical data for the transverse mass spectra of Helium-3 in rapidity interval

Numerical data for the transverse mass spectra of Helium-3 in rapidity interval

Numerical data for the transverse mass spectra of Helium-3 in rapidity interval

Numerical data for the transverse mass spectra of Helium-3 in rapidity interval

Numerical data for the transverse mass spectra of Helium-3 in rapidity interval

Numerical data for the transverse mass spectra of Helium-3 in rapidity interval

Numerical data for the transverse mass spectra of Helium-3 in rapidity interval

Numerical data for the transverse mass spectra of Helium-3 in rapidity interval

Numerical data for the transverse mass spectra of Helium-3 in rapidity interval

Numerical data for the transverse mass spectra of Helium-3 in rapidity interval

Numerical data for the transverse mass spectra of Helium-3 in rapidity interval

Numerical data for the transverse mass spectra of Helium-3 in rapidity interval

Numerical data for the transverse mass spectra of Helium-3 in rapidity interval

Numerical data for the transverse mass spectra of Helium-3 in rapidity interval

Numerical data for the transverse mass spectra of Helium-3 in rapidity interval

Numerical data for the transverse mass spectra of Helium-3 in rapidity interval

Numerical data for the transverse mass spectra of Helium-3 in rapidity interval

Numerical data for the transverse mass spectra of Helium-3 in rapidity interval

Numerical data for the transverse mass spectra of Helium-3 in rapidity interval

Numerical data for the transverse mass spectra of Helium-3 in rapidity interval

Numerical data for the transverse mass spectra of tritium in rapidity interval

Numerical data for the transverse mass spectra of tritium in rapidity interval

Numerical data for the transverse mass spectra of tritium in rapidity interval

Numerical data for the transverse mass spectra of tritium in rapidity interval

Numerical data for the transverse mass spectra of tritium in rapidity interval

Numerical data for the transverse mass spectra of deuterim in rapidity interval

Numerical data for the transverse mass spectra of deuterim in rapidity interval

Numerical data for the transverse mass spectra of deuterim in rapidity interval

Numerical data for the transverse mass spectra of deuterim in rapidity interval

Numerical data for the transverse mass spectra of deuterim in rapidity interval

Numerical data for the coalescence parameter B2 of deuterons in rapidity interval

Numerical data for the coalescence parameter B2 of deuterons in rapidity interval

Numerical data for the coalescence parameter B2 of deuterons in rapidity interval

Numerical data for the coalescence parameter B2 of deuterons in rapidity interval

Numerical data for the coalescence parameter B2 of deuterons in rapidity interval

Numerical data for the coalescence parameter B3 of helium-3 in rapidity interval

Numerical data for the coalescence parameter B3 of helium-3 in rapidity interval

Numerical data for the coalescence parameter B3 of helium-3 in rapidity interval

Numerical data for the coalescence parameter B3 of helium-3 in rapidity interval

Numerical data for the coalescence parameter B3 of helium-3 in rapidity interval

Transverse momentum spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 20 GeV in various rapidity ranges.

Transverse momentum spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 31 GeV in various rapidity ranges.

Transverse momentum spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 31 GeV in various rapidity ranges.

Transverse momentum spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 31 GeV in various rapidity ranges.

Transverse momentum spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 31 GeV in various rapidity ranges.

Transverse momentum spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 40 GeV in various rapidity ranges.

Transverse momentum spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 40 GeV in various rapidity ranges.

Transverse momentum spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 40 GeV in various rapidity ranges.

Transverse momentum spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 40 GeV in various rapidity ranges.

Transverse momentum spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 80 GeV in various rapidity ranges.

Transverse momentum spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 80 GeV in various rapidity ranges.

Transverse momentum spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 80 GeV in various rapidity ranges.

Transverse momentum spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 80 GeV in various rapidity ranges.

Transverse momentum spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 80 GeV in various rapidity ranges.

Transverse momentum spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 158 GeV in various rapidity ranges.

Transverse momentum spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 158 GeV in various rapidity ranges.

Transverse momentum spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 158 GeV in various rapidity ranges.

Transverse momentum spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 158 GeV in various rapidity ranges.

Transverse momentum spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 158 GeV in various rapidity ranges.

Transverse mass spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 20 GeV in various rapidity ranges.

Transverse mass spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 20 GeV in various rapidity ranges.

Transverse mass spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 20 GeV in various rapidity ranges.

Transverse mass spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 20 GeV in various rapidity ranges.

Transverse mass spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 31 GeV in various rapidity ranges.

Transverse mass spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 31 GeV in various rapidity ranges.

Transverse mass spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 31 GeV in various rapidity ranges.

Transverse mass spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 31 GeV in various rapidity ranges.

Transverse mass spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 40 GeV in various rapidity ranges.

Transverse mass spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 40 GeV in various rapidity ranges.

Transverse mass spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 40 GeV in various rapidity ranges.

Transverse mass spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 40 GeV in various rapidity ranges.

Transverse mass spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 80 GeV in various rapidity ranges.

Transverse mass spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 80 GeV in various rapidity ranges.

Transverse mass spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 80 GeV in various rapidity ranges.

Transverse mass spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 80 GeV in various rapidity ranges.

Transverse mass spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 158 GeV in various rapidity ranges.

Transverse mass spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 158 GeV in various rapidity ranges.

Transverse mass spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 158 GeV in various rapidity ranges.

Transverse mass spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 158 GeV in various rapidity ranges.

Transverse mass spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 158 GeV in various rapidity ranges.

Inverse slope parameter T as a function of rapidity for the 5 beam momenta.

Rapidity spectra for the 5 beam momenta.

Mean transverse mass as a function of rapidity for the 5 beam momenta.

Numerical values of the parameters fitted to the rapidiy distributions.