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The asymmetry of baryon/antibaryon production has been measured in manyproton-proton, pion-proton and electron-proton experiments. In the framework ofQuark-Gluon String Model (QGSM) the energy dependence of asymmetry tells usabout the value of $\alpha_{SJ}$(0), the intercept of String Junction Reggetrajectory. In previous QGSM study, the value of intercept has been estimatedas 0.5 < $\alpha_{SJ}$(0) < 0.9. Here, SJ behaviors are accumulated in themodel based on topological expansion in order to build a neutral object withzero baryon charge. By the way, QCD mass falling under the event horizon ofBlack Hole (BH) should be symmetric, or in other words, have no chargeinformation. The baryon junctions are easily combinable with antibaryon ones inhexagons. Topologically, hexagon net can coherently cover only the torussurface. The net on the torus has discrete number of baryon/antibaryonjunctions. This is only parameter that marks the mass/energy level of thisobject. It looks like DM particle, is not it? In high energy collisions at LHC,such pomeron loops are to be produced approximately in 1.2 percent of inelasticevents. Furthermore, the torus configurations of matter have been revealed inmany bright events in space. As an example, Chandra experiment has detectedsuch dense "doughnut" near the event horizon of Super Massive Black Hole(SMBH), which X-ray radiation is screened on 40 percent's. This topologicalsymmetry model of DM seems rather realistic and can help us to deal with an"arm wrestling" between the stiffness of toroid structure of QCD matter and thepressure of gravitational singularity at extremely heavy masses. On the otherhand, the instabilities in structure of matter in SMBHs can cause the bursts ofgiant relativistic hadron jets with the masses of order the own BH mass.

Baryon-antiBaryon Charge Asymmetry at LHC: String Junction Transfer and SJ Torus as DM Candidate