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Bulletin of the American Physical Society

Quantum spin state in a spin-1/2 breathing pyrochlore antiferromagnet

Kenta Kimura, Satoru Nakatsuji, T. Kimura

Published Mar 3, 2015• 0 citations
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arXiv:1710.11316•Physical review. B./Physical review. B•Apr 12, 2018•19 citations
Geometric frustration in spin systems offers potential routes to realize unusual phases of matter. The authors consider emergent quantum spin liquids of interacting S=1/2S=1/2S=1/2 moments on the pyrochlore lattice with a breathing anisotropy, where two inequivalent sets of tetrahedra are present. They classify possible Z2{\mathbb{Z}}_{2}Z2​ and U(1) quantum spin liquids in this system and find a small number of physically motivated candidates. In particular, two degenerate U(1) spin liquids are identified for the antiferromagnetic Heisenberg model. The degeneracy is robust with respect to tuning the breathing anisotropy, but it can be lifted by a finite Dzyaloshinskii-Moriya interaction. The effect of gauge fluctuations in a gapless U(1) spin liquid is investigated for comparison with future experiments.
We present exact diagonalization calculations for the spin-1/2 nearest-neighbor antiferromagnet on the pyrochlore lattice. We study a section of the lattice in the [111] direction and analyze the Hamiltonian of the breathing pyrochlore system with two coupling constants J1{J}_{1}J1​ and J2{J}_{2}J2​ for tetrahedra of different orientations and investigate the evolution of the system from the limit of disconnected tetrahedra (J2=0{J}_{2}=0J2​=0) to a correlated state at J1=J2{J}_{1}={J}_{2}J1​=J2​. We evaluate the low-energy spectrum, two and four spin correlations, and spin chirality correlations for a system size of up to 36 sites. The model shows a fast decay of spin correlations and we confirm the presence of several singlet excitations below the lowest magnetic excitation. We find chirality correlations near J1=J2{J}_{1}={J}_{2}J1​=J2​ to be small at the length scales available at this system size. Evaluation of dimer-dimer correlations and analysis of the nature of the entanglement of the tetrahedral unit shows that the triplet sector of the tetrahedron contributes significantly to the ground-state entanglement at J1=J2{J}_{1}={J}_{2}J1​=J2​.