Abstract

Using a variational Monte Carlo method, we discuss the interplay between antiferromagnetism (AF) and superconductivity (SC) in a Hubbard model on a square lattice with a diagonal transfer t ′ . We simultaneously introduce the following improvements into the trial function: (1) coexistence of AF and d-wave singlet gaps that allows a continuous description of their interplay, (2) band renormalization effect in the range of fourth-neighbor hopping, and (3) refined doublon–holon correlation factors. For t ′ / t = - 0.3 , appropriate to hole-doped cuprates, it is found that AF ordered state is stabilized near half filling, especially, for U ∼ band width, by retrieving the nesting condition. As the doping rate increases, AF is weakened and a pure d-wave SC phase evolves for large U. The coexisting state of SC and AF orders appears only in a narrow range of U ( ∼ band width) and electron density n ( = 0.8 ).

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