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Ground States of Spin-1/2 Heisenberg Antiferromagnets with Frustration on a Diamond-Like Decorated Square Lattice

We study the ground-state phase diagram of a Heisenberg model with spin $S=\frac{1}{2}$ on a diamond-like decorated square lattice. A diamond unit has two types of antiferromagnetic exchange interactions, and the ratio $λ$ between the length of the diagonal bond and that of the other four edges determines the strength of frustration. It has been pointed out [J. Phys. Soc. Jpn {\bf85}, 033705 (2016)] that the so-called tetramer-dimer states, which are expected to be stabilized in an intermediate region of $λ_{\rm c}<λ<2$, are identical to the square-lattice dimer covering states, which ignited renewed interest in high-dimensional diamond-like decorated lattices. In order to determine the phase boundary $λ_{\rm c}$, we employ the modified spin wave method to estimate the energy of the ferrimagnetic state and obtain $λ_{\rm c}=0.974$. Our obtained magnetizations for spin-$\frac{1}{2}$ sites and for spin-1 sites are $m=0.398$ and $\tilde{m}=0.949$, and spin reductions are 20 \% and 5\%, respectively. This indicates that spin fluctuation is much smaller than that of the $S=\frac{1}{2}$ square-lattice antiferromagnet: thus, we can consider that our obtained ground-state energy is highly accurate. Further, our numerical diagonalization study suggests that other cluster states do not appear in the ground-state phase diagram.