“…whereĉ † i,µσ is the creation operator for electron with spin σ =↑, ↓ and orbital flavor µ = xy, yz, zx at site-i, ij µ indicates the nearest-neighbor (NN) pair along the 110 direction that corresponds to the active t 2g orbital µ, the hopping constant t is set to be 1 in all the simulations below, J ≈ U eff ŝ is the effective Hund's coupling, S i is the O(3) local magnetic moment, and s i,µ = α,β c † iµα σ αβ c iµβ is the electron spin operator. The 1D ferromagnetic Kondo chain, which is the backbone of Hamiltonian (1), have been extensively studied over the years [27][28][29]. However, the fact that every local spin S i is shared by three Kondo chains introduces competition between different chains.…”