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. 2019 Oct 1;52(10):2981–2993. doi: 10.1021/acs.accounts.9b00373

Figure 8.

Figure 8

(a) Schematic representation of di-EMFs with a single-electron Ln–Ln bond as a three-center [Ln3+–e–Ln3+] spin system. (b) Alignment of the Tb spins (green arrows) and the unpaired electron spin (red arrow) in Tb2@C79N. (c) Alignment of the Ln and unpaired electron spins (red arrows) in {Ln2} molecules. The spins of Er ions are visualized as ellipsoids built upon the g tensors of their single-ion ground states. (d) Low-energy spectrum of the spin Hamiltonian (eq 6) for {Tb2} with Keff = 55 cm–1. Red lines visualize transition probabilities. Tb and unpaired spins are shown with green and red arrows, respectively. Dashed arrows show the QTM and Orbach mechanisms.