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.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0003 and Q^2=8.5 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0003 and Q^2=12.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0010 and Q^2=3.5 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0010 and Q^2=5.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0010 and Q^2=6.5 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0010 and Q^2=8.5 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0010 and Q^2=12.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0010 and Q^2=15.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0010 and Q^2=20.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0010 and Q^2=25.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0010 and Q^2=35.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0010 and Q^2=45.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0030 and Q^2=3.5 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0030 and Q^2=5.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0030 and Q^2=6.5 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0030 and Q^2=8.5 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0030 and Q^2=12.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0030 and Q^2=15.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0030 and Q^2=20.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0030 and Q^2=25.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0030 and Q^2=35.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0030 and Q^2=45.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0030 and Q^2=60.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0030 and Q^2=90.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0100 and Q^2=3.5 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0100 and Q^2=5.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0100 and Q^2=6.5 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0100 and Q^2=8.5 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0100 and Q^2=12.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0100 and Q^2=15.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0100 and Q^2=20.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0100 and Q^2=25.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0100 and Q^2=35.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0100 and Q^2=45.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0100 and Q^2=60.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0100 and Q^2=90.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0100 and Q^2=200.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0100 and Q^2=400.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0300 and Q^2=3.5 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0300 and Q^2=5.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0300 and Q^2=6.5 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0300 and Q^2=8.5 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0300 and Q^2=12.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0300 and Q^2=15.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0300 and Q^2=20.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0300 and Q^2=25.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0300 and Q^2=35.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0300 and Q^2=45.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0300 and Q^2=60.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0300 and Q^2=90.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0300 and Q^2=200.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0300 and Q^2=400.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0300 and Q^2=800.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

The reduced diffractive cross section multiplied by X_Pomeron at XP=0.0300 and Q^2=1600.0 GeV^2 . The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

Double-differential trijet cross sections measured as a function of Q**2 and MEAN(PT(3JET)) using the kT jet algorithm. The total systematic uncertainty sums all systematic uncertainties in quadrature, including the uncertainty due to the LAr noise of 0.9% and the total normalisation uncertainty of 2.9%. The correction factors on the theoretical cross sections C(HAD) and C(EW) are listed in the rightmost columns.

Double-differential trijet cross sections measured as a function of Q**2 and XI(3) using the kT jet algorithm. The total systematic uncertainty sums all systematic uncertainties in quadrature, including the uncertainty due to the LAr noise of 0.9% and the total normalisation uncertainty of 2.9%. The correction factors on the theoretical cross sections C(HAD) and C(EW) are listed in the rightmost columns.

Double-differential inclusive jet cross sections measured as a function of Q**2 and PT(JET) using the anti-kT jet algorithm. The total systematic uncertainty sums all systematic uncertainties in quadrature, including the uncertainty due to the LAr noise of 0.5% and the total normalisation uncertainty of 2.9%. The correction factors on the theoretical cross sections C(HAD) and C(EW) are listed in the rightmost columns.

Double-differential dijet cross sections measured as a function of Q**2 and MEAN(PT(2JET)) using the anti-kT jet algorithm. The total systematic uncertainty sums all systematic uncertainties in quadrature, including the uncertainty due to the LAr noise of 0.6% and the total normalisation uncertainty of 2.9%. The correction factors on the theoretical cross sections C(HAD) and C(EW) are listed in the rightmost columns.

Double-differential dijet cross sections measured as a function of Q**2 and XI(2) using the anti-kT jet algorithm. The total systematic uncertainty sums all systematic uncertainties in quadrature, including the uncertainty due to the LAr noise of 0.6% and the total normalisation uncertainty of 2.9%. The correction factors on the theoretical cross sections C(HAD) and C(EW) are listed in the rightmost columns.

Double-differential trijet cross sections measured as a function of Q**2 and MEAN(PT(3JET)) using the anti-kT jet algorithm. The total systematic uncertainty sums all systematic uncertainties in quadrature, including the uncertainty due to the LAr noise of 0.9% and the total normalisation uncertainty of 2.9%. The correction factors on the theoretical cross sections C(HAD) and C(EW) are listed in the rightmost columns.

Double-differential trijet cross sections measured as a function of Q**2 and XI(3) using the anti-kT jet algorithm. The total systematic uncertainty sums all systematic uncertainties in quadrature, including the uncertainty due to the LAr noise of 0.9% and the total normalisation uncertainty of 2.9%. The correction factors on the theoretical cross sections C(HAD) and C(EW) are listed in the rightmost columns.

Double-differential normalised inclusive jet cross sections measured as a function of Q**2 and PT(JET) using the kT jet algorithm. The total systematic uncertainty sums all systematic uncertainties in quadrature, including the uncertainty due to the LAr noise of 0.5% and the total normalisation uncertainty of 2.9%. The correction factors on the theoretical cross sections C(HAD) and C(EW) are listed in the rightmost columns.

Double-differential normalised dijet cross sections measured as a function of Q**2 and MEAN(PT(2JET)) using the kT jet algorithm. The total systematic uncertainty sums all systematic uncertainties in quadrature, including the uncertainty due to the LAr noise of 0.6% and the total normalisation uncertainty of 2.9%. The correction factors on the theoretical cross sections C(HAD) and C(EW) are listed in the rightmost columns.

Double-differential normalised inclusive dijet cross sections measured as a function of Q**2 and XI(2) using the kT jet algorithm. The total systematic uncertainty sums all systematic uncertainties in quadrature, including the uncertainty due to the LAr noise of 0.6% and the total normalisation uncertainty of 2.9%. The correction factors on the theoretical cross sections C(HAD) and C(EW) are listed in the rightmost columns.

Double-differential normalised trijet cross sections measured as a function of Q**2 and MEAN(PT(3JET)) using the kT jet algorithm. The total systematic uncertainty sums all systematic uncertainties in quadrature, including the uncertainty due to the LAr noise of 0.9% and the total normalisation uncertainty of 2.9%. The correction factors on the theoretical cross sections C(HAD) and C(EW) are listed in the rightmost columns.

Double-differential normalised trijet cross sections measured as a function of Q**2 and XI(3) using the kT jet algorithm. The total systematic uncertainty sums all systematic uncertainties in quadrature, including the uncertainty due to the LAr noise of 0.9% and the total normalisation uncertainty of 2.9%. The correction factors on the theoretical cross sections C(HAD) and C(EW) are listed in the rightmost columns.

Double-differential normalised inclusive jet cross sections measured as a function of Q**2 and PT(JET) using the anti-kT jet algorithm. The total systematic uncertainty sums all systematic uncertainties in quadrature, including the uncertainty due to the LAr noise of 0.5% and the total normalisation uncertainty of 2.9%. The correction factors on the theoretical cross sections C(HAD) and C(EW) are listed in the rightmost columns.

Double-differential normalised dijet cross sections measured as a function of Q**2 and MEAN(PT(2JET)) using the anti-kT jet algorithm. The total systematic uncertainty sums all systematic uncertainties in quadrature, including the uncertainty due to the LAr noise of 0.6% and the total normalisation uncertainty of 2.9%. The correction factors on the theoretical cross sections C(HAD) and C(EW) are listed in the rightmost columns.

Double-differential normalised inclusive dijet cross sections measured as a function of Q**2 and XI(2) using the anti-kT jet algorithm. The total systematic uncertainty sums all systematic uncertainties in quadrature, including the uncertainty due to the LAr noise of 0.6% and the total normalisation uncertainty of 2.9%. The correction factors on the theoretical cross sections C(HAD) and C(EW) are listed in the rightmost columns.

Double-differential normalised trijet cross sections measured as a function of Q**2 and MEAN(PT(3JET)) using the anti-kT jet algorithm. The total systematic uncertainty sums all systematic uncertainties in quadrature, including the uncertainty due to the LAr noise of 0.9% and the total normalisation uncertainty of 2.9%. The correction factors on the theoretical cross sections C(HAD) and C(EW) are listed in the rightmost columns.

Double-differential normalised trijet cross sections measured as a function of Q**2 and XI(3) using the anti-kT jet algorithm. The total systematic uncertainty sums all systematic uncertainties in quadrature, including the uncertainty due to the LAr noise of 0.9% and the total normalisation uncertainty of 2.9%. The correction factors on the theoretical cross sections C(HAD) and C(EW) are listed in the rightmost columns.

The proton-dissociative photoproduction cross section derived from the low-energy data set as a function of the photon-proton centre-of-mass energy W. PHI_T is the transeverse polarised photon flux.

The elastic photoproduction differential cross section derived from the high-energy data set as a function of the negative squared momentum transfer at the proton vertex T.

The proton-dissociative photoproduction differential cross section derived from the high-energy data set as a function of the negative squared momentum transfer at the proton vertex T.

The elastic photoproduction differential cross section derived from the low-energy data set as a function of the negative squared momentum transfer at the proton vertex T.

The proton-dissociative photoproduction differential cross section derived from the low-energy data set as a function of the negative squared momentum transfer at the proton vertex T.

Differential cross section of elastic $\pi^+$p-scattering at P= 810.75 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 814.54 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 818.13 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 822.17 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 825.83 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 829.92 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 833.58 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 837.67 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 841.33 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 845.17 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 848.83 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 852.67 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 856.33 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 859.96 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 863.71 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 867.58 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 871.42 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 874.88 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 878.79 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 882.50 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 886.50 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 890.00 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 894.00 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 897.50 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 901.50 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 905.00 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 909.00 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 912.50 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 916.50 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 919.04 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 923.38 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 927.33 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 931.92 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 936.25 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 940.58 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 948.08 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 952.75 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 957.42 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 963.33 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 968.00 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 972.67 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 978.33 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 983.00 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 987.67 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 993.58 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P= 998.25 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1002.92 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1008.58 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1013.25 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1017.92 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1023.58 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1028.25 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1032.92 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1038.58 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1043.25 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1047.92 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1053.58 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1058.25 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1062.92 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1068.58 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1073.25 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1077.92 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1083.33 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1088.00 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1092.67 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1097.83 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1102.50 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1107.17 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1111.83 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1116.50 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1121.17 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1125.83 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1130.50 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1135.17 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1139.83 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1144.50 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1149.17 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1154.83 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1159.50 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1164.17 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1170.83 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1175.50 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1180.17 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1186.33 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1191.00 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1195.67 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1201.33 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1206.00 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1210.67 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1216.33 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1221.00 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1225.67 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1231.17 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1236.00 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1240.83 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1247.00 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1252.00 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1257.00 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1262.00 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1267.00 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1272.00 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1276.50 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1281.50 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1286.50 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1291.50 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1296.50 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1301.50 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1306.00 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1311.00 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1316.00 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1320.50 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1325.50 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^+$p-scattering at P=1330.50 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 800.25 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 803.75 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 807.25 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 810.75 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 814.54 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 818.13 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 822.17 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 825.83 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 829.92 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 833.58 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 837.67 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 841.33 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 845.17 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 848.83 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 852.67 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 856.33 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 859.96 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 863.71 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 867.58 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 871.42 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 874.88 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 878.79 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 882.50 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 886.50 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 890.00 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 894.00 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 897.50 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 901.50 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 905.00 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 909.00 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 912.50 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 916.50 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 919.75 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 923.75 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 927.00 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 931.00 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 934.75 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 938.17 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 940.75 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 943.21 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 946.79 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 950.00 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 953.44 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 956.75 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 960.58 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 964.17 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 968.08 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 971.67 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 975.58 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 979.29 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 983.19 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 986.85 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 990.63 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 993.92 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P= 998.00 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1001.54 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1005.71 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1008.25 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1010.92 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1014.50 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1017.79 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1022.13 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1026.21 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1029.00 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1032.00 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1035.96 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1039.54 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1043.77 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1047.48 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1052.33 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1056.50 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1060.42 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1063.50 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1066.58 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1070.42 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1074.35 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1078.23 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1082.29 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1086.21 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1090.04 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1093.96 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1098.04 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1102.29 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1104.92 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1108.21 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1112.58 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1116.92 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1120.83 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1124.08 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1127.77 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1132.23 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1134.75 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1137.44 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1140.33 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1143.60 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1147.81 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1152.02 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1157.50 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1162.50 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1167.50 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1172.29 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1177.38 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1182.46 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1187.33 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1192.50 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1197.67 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1202.58 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1207.75 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1212.92 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1217.02 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1222.31 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1227.60 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1232.38 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1237.63 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1242.88 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1247.00 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1252.00 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1257.00 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1262.00 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1267.00 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1272.00 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1276.50 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1281.50 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1286.50 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1291.50 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1296.50 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1301.50 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1306.00 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1311.00 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1316.00 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1320.50 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1325.50 MeV/c. Errors shown are statistical only.

Differential cross section of elastic $\pi^-$p-scattering at P=1330.50 MeV/c. Errors shown are statistical only.

The combined differential cross sections (DSIG/DET,OUT) separately for the low and high Q**2 regions. The data are corrected using the HERWIG-kt model.

The combined differential cross sections (DSIG/DET,OUT) separately for the low and high Q**2 regions. The data are corrected using the PHOJET model.

The combined differential cross sections (DSIG/DN,TRK) separately for the low and high Q**2 regions. The data are corrected using the HERWIG-kt model.

The combined differential cross sections (DSIG/DN,TRK) separately for the low and high Q**2 regions. The data are corrected using the PHOJET model.

The combined differential cross sections (DSIG/DPT,TRK) separately for the low and high Q**2 regions. The data are corrected using the HERWIG-kt model.

The combined differential cross sections (DSIG/DPT,TRK) separately for the low and high Q**2 regions. The data are corrected using the PHOJET model.

The combined energy flow (DE/DETARAP) separately for the low and high Q**2 regions. The data are corrected using the HERWIG-kt model.

The combined energy flow (DE/DETARAP) separately for the low and high Q**2 regions. The data are corrected using the PHOJET model.

Integrated EP cross section.

Integrated EP cross section.

GAMMA* P cross section.

GAMMA* P cross section.

GAMMA* P cross section.

Numerical values modified in the Erratum.

No description provided.

No description provided.

The systematic error is estimated by varying the background contributions by one standard deviation and their slopes between 0 and 3 Gev**-2.

DATA ARE GIVEN ON GRAPHS ONLY.

Longitudinal to transverce cross section ratio.

Longitudinal to transverce cross section ratio.

Longitudinal to transverce cross section ratio in all range.

Cross section was fitted by Q2**POWER.

Cross section was fitted by D(SIG)/D(T)(T=0)*(M(P=3 4)**4)**POWER. Joint fit of H1 and NMC (see NP B429, 503 <a href=http://durpdg.dur.ac.uk/scripts/reacsearch.csh/TESTREAC/red+3112> RED = 3112 </a>) data. An overall 20 PCT normalization uncertainty in NMC data included.

Cross section was fitted by 1/(Q2+M(j/psi)**2)**POWER.

No description provided.

Normalised cross sections of forward neutron production in DIS as a function of XF. For each measurement, the statistical, the uncorrelated systematic uncertainties and the bin-to-bin correlated systematic uncertainties due to the FNC absolute energy scale (EFNC), the measurement of the particle impact position in the FNC (XYFNC) and the model dependence of the data correction (model) are given.

Bin averaged hadron level differential cross section for diffractive dijet production as a function of X(C=POMERON). The first systematic error is the uncorrelated and the second the correlated uncertainty.

Bin averaged hadron level differential cross section for diffractive dijet production as a function of Z(C=POMERON). The first systematic error is the uncorrelated and the second the correlated uncertainty.

Bin averaged hadron level differential cross section for diffractive dijet production as a function of the average pseudorapidity of the dijet system. The first systematic error is the uncorrelated and the second the correlated uncertainty.

Bin averaged hadron level differential cross section for diffractive dijet production as a function of the absolute difference of the pseudorapidities of the two jets. The first systematic error is the uncorrelated and the second the correlated uncertainty.

Bin averaged hadron level differential cross section for diffractive dijet production as a function of W. The first systematic error is the uncorrelated and the second the correlated uncertainty.

Bin averaged hadron level differential cross section for diffractive dijet production as a function of the dijet invariant mass. The first systematic error is the uncorrelated and the second the correlated uncertainty.

Bin averaged hadron level differential cross section for diffractive dijet production as a function of mass of the diffractive system. The first systematic error is the uncorrelated and the second the correlated uncertainty.

Bin averaged hadron level double-differential cross section for diffractive dijet production as a function of X(GAMMA) for 3 ranges of ET of jet 1. The first systematic error is the uncorrelated and the second the correlated uncertainty.

Bin averaged hadron level double-differential cross section for diffractive dijet production as a function of Z(POMERON) for 2 ranges of X(GAMMA). The first systematic error is the uncorrelated and the second the correlated uncertainty.

Ratios of the diffractive to the inclusive single-differential hadron level dijet cross sections as a function of X(C=GAMMA). The first systematic error is the uncorrelated and the second the correlated uncertainty.

Ratios of the diffractive to the inclusive single-differential hadron level dijet cross sections as a function of ET of jet 1. The first systematic error is the uncorrelated and the second the correlated uncertainty.

Ratios of the diffractive to the inclusive single-differential hadron level dijet cross sections as a function of the average pseudorapidity of the dijet system. The first systematic error is the uncorrelated and the second the correlated uncertainty.

Ratios of the diffractive to the inclusive single-differential hadron level dijet cross sections as a function of the absolute difference in the pseudorapidities of the 2 jets. The first systematic error is the uncorrelated and the second the correlated uncertainty.

Ratios of the diffractive to the inclusive single-differential hadron level dijet cross sections as a function of the invariant mass of the dijet system. The first systematic error is the uncorrelated and the second the correlated uncertainty.

Ratios of the diffractive to the inclusive single-differential hadron level dijet cross sections as a function of W. The first systematic error is the uncorrelated and the second the correlated uncertainty.