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. 2023 May 30;14:3134. doi: 10.1038/s41467-023-38431-7

Fig. 1. Competing interactions in Pr4+ oxides.

Fig. 1

a Hierarchy of single-ion energy scales for Pr4+ ions in octahedral oxygen environments starting from a 2F, (S = 1/2, L = 3) free-ion state. For spin-orbit coupling (SOC) as the dominant energy scale (Jeff = 1/2 limit, left, brown), the low-symmetry crystal field (CF) lifts the degeneracy of the ground-state 2F5/2 and excited 2F7/2 multiplets into seven Kramers doublets (KDs, with selected radial squared wave-functions represented). For approximate Oh symmetry, the Γ7 doublet, in the J,mJ basis, is given by Γ7±=sinθ52,±52+cosθ52,32, where sin2θ1/6 (See SI). For CF as the dominant energy scale (Seff = 1/2 limit, right, blue), SOC and distortion from Oh symmetry lift the 2A2u ground state and the triply degenerate 2T2u and 2T1u excited states into seven KDs. The ground-state doublet is given in the ml,ms basis by ±=A3,±12B2,12+C±1,±12D±2,12, where (A2/B2)Γ72.6 and (C2/D2)Γ70.33 for the Γ7 doublet62 (See SI). In the intermediate limit, the competition between ΔCF and ζSOC scales in Pr4+ yields seven KD (indicated by the mix of brown/blue lines) with magnetic properties that are distinct from the Jeff = 1/2 and Seff = 1/2 limits, such as large magnetic super-exchange achievable by tuning the ligand field. bd Crystal structure, magnetic lattice dimensionality, and Pr4+ coordination environment for the oxides studied in this work: Na2PrO3 (2-Pr), Sr2PrO4 (1-Pr), and Li8PrO6 (0-Pr), respectively.