Erratum: Three-jet production and gluon saturation effects in $p-p$ and $p$-Pb collisions within high-energy factorization [Phys. Rev. D 88, 094001 (2013)]

Figure 1

Differential cross section in the difference of the azimuthal angles between the leading and forward jets. The band represents the theoretical uncertainty due to scale variation and statistical errors. The left plot corresponds to a center-of-mass energy of 5.02 TeV, the right to one of 7.0 TeV.

Figure 2

The nuclear modification factor as a function of the difference of the azimuthal angles between the leading and forward jets. The band represents the theoretical uncertainty due to scale variation and statistical errors. The left plot corresponds to a center-of-mass energy of 5.02 TeV, the right to one of 7.0 TeV.

Figure 3

Differential cross section in the difference of the azimuthal angles between the leading and forward jets for the particular choice of the scale $\mu /2$. The left column corresponds to a center-of-mass energy of 5.02 TeV, the right to one of 7.0 TeV.

Figure 4

Differential cross section in the difference of the azimuthal angles between the leading and forward jets, with the additional restriction that the two leading jets are back-to-back-like. The band represents the theoretical uncertainty due to scale variation and statistical errors. The left plot corresponds to a center-of-mass energy of 5.02 TeV, the right to one of 7.0 TeV.

Figure 5

The nuclear modification factor as a function of the difference of the azimuthal angles between the leading and forward jets, with the additional restriction that the two leading jets are back-to-back-like. The band represents the theoretical uncertainty due to scale variation and statistical errors. The left plot corresponds to a center-of-mass energy of 5.02 TeV, the right to one of 7.0 TeV.

Figure 6

Differential cross section in the difference of the azimuthal angles between the leading and forward jets, with the additional restriction that the two leading jets are back-to-back-like. The left plot corresponds to a center-of-mass energy of 5.02 TeV, the right to one of 7.0 TeV. The plots are made for the particular choice of the scale equal to $\mu /2$.

Figure 7

Differential cross section in the difference of the azimuthal angles between the leading and forward jets for the forward rapidity region. The band represents the theoretical uncertainty due to scale variation and statistical errors. The left plot corresponds to a center-of-mass energy of 5.02 TeV, the right to one of 7.0 TeV.

Figure 8

The nuclear modification factor as a function of the difference of the azimuthal angles between the leading and forward jets for the forward rapidity region. The band represents the theoretical uncertainty due to scale variation and statistical errors. The left plot corresponds to a center-of-mass energy of 5.02 TeV, the right to one of 7.0 TeV.

Figure 9

Differential cross section in the difference of the azimuthal angles between the leading and forward jets for the forward rapidity region. The left plot corresponds to a center-of-mass energy of 5.02 TeV, the right to one of 7.0 TeV. The plots are made for the particular choice of the scale equal to $\mu /2$.