Abstract
Controlling properties within a given functional inorganic material structure type is often accomplished through tuning the electronic occupation, which is in turn dictated by the elemental composition determined at the time of material preparation. We employ electrochemical control of the lithium content, with associated electronic occupancy control, to vary the magnetic properties of a material where a kagome-derived network of Mo3 triangles carry the spin. In this case, Li is electrochemically inserted into LiScMo3O8, a layered compound containing a breathing Mo kagome network. Up to two additional Li can be inserted into LiScMo3O8, transforming it into Li3ScMo3O8. Li2ScMo3O8 prepared by electrochemical lithiation is compared to the quantum spin liquid candidate compound Li2ScMo3O8 prepared through high-temperature solid-state methods, which has a slightly different structural stacking sequence but a similar kagome-derived network. Magnetic measurements are supported by first-principles calculations, showing that electrons remain localized on the Mo clusters throughout the doping series. As x is varied in LixScMo3O8, the measurements and calculations reveal the evolution from a diamagnetic band insulator at x = 1 to a geometrically frustrated magnet at x = 2, back to a diamagnetic insulator at x = 3. These results indicate a likelihood of strong coupling between the degree of Li disorder and charge/magnetic ordering over the Mo3 clusters.
Original language | English |
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Pages (from-to) | 4945-4954 |
Number of pages | 10 |
Journal | Chemistry of Materials |
Volume | 35 |
Issue number | 13 |
DOIs | |
State | Published - Jul 11 2023 |
Funding
This work was supported as part of the Center for Synthetic Control Across Length scales for Advancing Rechargeables (SCALAR), an Energy Frontier Research Center funded by the U.S. Department of Energy, Office of Science, Basic Energy Sciences under Award DE SC0019381. This research used computational resources of the National Energy Research Scientific Computing Center (NERSC), a U.S. Department of Energy Office of Science User Facility located at Lawrence Berkeley National Laboratory, operated under Contract No. DE-AC02-05CH11231, and shared facilities of the UC Santa Barbara Materials Research Science and Engineering Center (MRSEC, NSF DMR 1720256), a member of the Materials Research Facilities Network (www.mrfn.org). We also acknowledge use of the shared computing facilities of the Center for Scientific Computing at UC Santa Barbara, supported by NSF CNS-1725797, and the NSF MRSEC at UC Santa Barbara, NSF DMR 1720256. We gratefully acknowledge support via the UC Santa Barbara NSF Quantum Foundry funded via the Q-AMASE-i program under award DMR-1906325. J.L.K. acknowledges support from the U.S. Department of Energy, Office of Science, Office of Advanced Scientific Computing Research, Department of Energy Computational Science Graduate Fellowship under Award Number DE-FG02-97ER25308. This research used resources of the Advanced Photon Source, a U.S. Department of Energy (DOE) Office of Science user facility operated for the DOE Office of Science by Argonne National Laboratory under Contract No. DE-AC02-06CH11357. A portion of this research used resources at the High Flux Isotope Reactor and the Spallation Neutron Source, a DOE Office of Science User Facility operated by the Oak Ridge National Laboratory. This work was supported as part of the Center for Synthetic Control Across Length scales for Advancing Rechargeables (SCALAR), an Energy Frontier Research Center funded by the U.S. Department of Energy, Office of Science, Basic Energy Sciences under Award DE SC0019381. This research used computational resources of the National Energy Research Scientific Computing Center (NERSC), a U.S. Department of Energy Office of Science User Facility located at Lawrence Berkeley National Laboratory, operated under Contract No. DE-AC02-05CH11231, and shared facilities of the UC Santa Barbara Materials Research Science and Engineering Center (MRSEC, NSF DMR 1720256), a member of the Materials Research Facilities Network ( www.mrfn.org ). We also acknowledge use of the shared computing facilities of the Center for Scientific Computing at UC Santa Barbara, supported by NSF CNS-1725797, and the NSF MRSEC at UC Santa Barbara, NSF DMR 1720256. We gratefully acknowledge support via the UC Santa Barbara NSF Quantum Foundry funded via the Q-AMASE-i program under award DMR-1906325. J.L.K. acknowledges support from the U.S. Department of Energy, Office of Science, Office of Advanced Scientific Computing Research, Department of Energy Computational Science Graduate Fellowship under Award Number DE-FG02-97ER25308. This research used resources of the Advanced Photon Source, a U.S. Department of Energy (DOE) Office of Science user facility operated for the DOE Office of Science by Argonne National Laboratory under Contract No. DE-AC02-06CH11357. A portion of this research used resources at the High Flux Isotope Reactor and the Spallation Neutron Source, a DOE Office of Science User Facility operated by the Oak Ridge National Laboratory.
Funders | Funder number |
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Center for Scientific Computing at UC Santa Barbara | CNS-1725797 |
Department of Energy Computational Science | DE-FG02-97ER25308 |
NSF DMR | 1720256 |
UC Santa Barbara Materials Research Science and Engineering Center | |
UC Santa Barbara NSF | DMR-1906325 |
National Science Foundation | DMR 1720256 |
U.S. Department of Energy | |
Office of Science | |
Basic Energy Sciences | DE SC0019381 |
Advanced Scientific Computing Research | |
Argonne National Laboratory | DE-AC02-06CH11357 |
Oak Ridge National Laboratory | |
Lawrence Berkeley National Laboratory | DE-AC02-05CH11231 |
University of California, Santa Barbara | |
Materials Research Science and Engineering Center, Harvard University |