“…Despite of their relative simplicity, the investigated mixed spin-electron models have proven to be suitable to simulate many unconventional physical properties and unusual cooperative phenomena with a good qualitative coincidence of the magnetic behavior of real materials. We can mention, for example, the kinetically-driven frustration of the Ising sub-lattice, [13][14][15][16][17][18][19][22][23][24] the local chirality in the electron sub-lattice, [15][16][17][18]22) rational 12-15, 17, 18, 23, 24, 28) and doping-dependent 17,19) magnetization plateaus in magnetization curves, double-and also triple-peak temperature dependences of the specific heat, 12-15, 22, 23) temperature-induced reentrant phase transitions, [26][27][28]31) the bipartite fermionic entanglement between mobile electrons, 20,21,24) and, last but not least, also the enhanced magnetocaloric 16,18) or magnetoelec-tric 29,30,32) effects.…”