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Large scale chromomagnetic, B_3, B_8, and usual magnetic,H, fields have to begenerated in QCD after the deconfinement phase transition (DPT) at temperaturesT larger than deconfinement temperature T_d. The two former fields are createdspontaneously due to asymptotic freedom of gluon intaractions. Whereas H isproduced due to either the feature of quarks to possess both electric and colorcharges or a vacuum polarization in this case. At the polarization, the vacuumquark loops mix the external fields. As a result, B_3, B_8 become the sourcesgenerating H. The latter field appears at $T$ much lower than the electroweakphase transition temperature T_ew. This mechanism should exhibit itself at theLHC experiments on heavy ion collisions. It operates at the one-loop diagramlevel for an effective potential. The created fields are temperature dependentand occupying the macroscopic volume of quark-gluon plasma. The magnetizationinfluences different processes and may serve as a signal for the DPT.

On magnetization of quark-gluon plasma at the LHC experiment energies