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Fractional excitations offer vast potential for both fundamental physics and quantum technologies. However, their dynamics under the influence of gauge fields pose a significant challenge to conventional models. Here, we investigate the evolution of low-energy Majorana dispersions across various crystalline phases of the -flux in the Kitaev spin model on a honeycomb lattice. We develop an effective tight-binding description for these low-energy Majorana fermions, introducing a gauge potential through a superexchange-like interaction that systematically eliminates the high-energy spectrum. We identify conditions under which this superexchange interaction acts as a Z2 gauge field, governing the tight-binding hopping of Majorana Wannier orbitals. Our study reveals an intriguing phase transition between two non-trivial topological phases characterized by gapless flat-band (extensive) degeneracy. To further explore flat band physics, we introduce a mean-field theory describing a gauge-invariant Majorana density-wave order within these bands. The resulting split Chern bands facilitate the partial filling of Chern bands, effectively leading to fractional Chern states. Our work, encompassing both the gauge-mediated tight-binding model and the mean-field theory, opens doors for future exploration of U (1), SU (N) gauge-mediated tight-binding approach to other fractional or entangled Wannier excitations.
Yogendra et al. (Thu,) studied this question.