“…where t η and J η are the hoping amplitude and exchange coupling, respectively, for the nearest neighbors η, t η is the hoping amplitude for the next nearest neighbors η , C † lσ (C lσ ) creates (annihilates) an electron at site l with spin σ, S l is the spin operator with its components S x l , S y l , and S z l , and µ is the chemical potential. Following the previous analyses of the exotic features of cuprate superconductors with coexisting electronic nematicity 51,52,[56][57][58][59] , the next nearest-neighbor (NN) hoping amplitude in the t-J model (1) is chosen as t τ = t , while the NN hoping amplitude t η can be chosen as,…”