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Experimental and theoretical premises of new stable hadron existence

“…are stable, at that the doublet of particles (M 0 , M − ) was named erzion in [16]. The states in Table 1 were also considered in [29] and [30] where U-type quark is contained in 4-th generation.…”

“…The charge M − and neutral M 0 particles can manifest themselves in Cosmic rays and as carrier of DM. In the work [16] these particles were considered in the frame-work of Erzion Model (see, olso, the fifth and sixth sections of this work), where neutral particles were called erzion and enion.…”

“…We, olso, assume that m D > m U + m e in the first mirror quark generation, that is new quark U is stable and D can be metastable. In this case, the neutral stable and charge metastable hadron states appear which are represented in the Table 1 (some of these hadrons were called erzion and enion in [16]) . As was shown in the second section, the charge asymmetry for new hadrons should be inverse with respect to one for usual hadrons.…”

“…In the framework of the already existing experimental programs on Cosmic rays physics [21] it is possible to conduct a targeted search for new particles, including new methods [14,22]. Systematical study of experimental and theoretical aspects of this problem are represented in a series of works, where experimental program search of new hadrons and their theoretical interpretation were considered [16], [23]- [28]. The possibilities of collider experiments also rise now due to their reaching higher energies.…”