“…There are different possibilities to have exotic baryon states: a) positive strangeness S > 0 (or negative charm C < 0, or positive beauty), since s-quark has S = −1 and c-quark C = +1, b) large (in modulus) negative strangeness S < −3B, B -baryon number; similar for charm or beauty, c) large enough isospin I > (3B + S)/2 , if −3B ≤ S ≤ 0, or charge Q > 2B + S or Q < −B in view of Gell-Mann -Nishijima relation Q = I 3 + Y /2. 1 Based partly on the talks presented at the International Seminar on High Energy Physics Quarks-2004, Pushkinogorie, Russia, May [24][25][26][27][28][29][30]2004; International Workshop on Quantum Field Theory and High Energy Physics QFTHEP-04, Saint-Petersburg, Russia, June [17][18][19][20][21][22][23]2004, and Symposium of London Mathematical Society "Topological Solitons and their Applications", Durham, UK, August 2- 12,2004. Slightly reduced version of this paper is available as E-print hep-ph/0507028.…”