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Magnetic order and spin liquid behavior in [Mo3]11+ molecular magnets

  • Q. Chen
  • , R. Sinclair
  • , A. Akbari-Sharbaf
  • , Q. Huang
  • , Z. Dun
  • , E. S. Choi
  • , M. Mourigal
  • , A. Verrier
  • , R. Rouane
  • , X. Bazier-Matte
  • , J. A. Quilliam
  • , A. A. Aczel
  • , H. D. Zhou

Research output: Contribution to journalArticlepeer-review

11 Scopus citations

Abstract

Molecular magnets based on [Mo3]11+ units with one unpaired electron per trimer have attracted recent interest due to the identification of quantum spin liquid candidacy in some family members. Here, we present comprehensive measurements on polycrystalline samples of ZnScMo3O8, MgScMo3O8, and Na3Sc2Mo5O16 with the same Mo3O13 magnetic building blocks. The crystal structures are characterized with x-ray or neutron powder diffraction and the magnetic ground states are determined by performing ac and dc susceptibility, specific heat, neutron powder diffraction, and muon spin relaxation measurements. Our work indicates that ZnScMo3O8 and MgScMo3O8 have ferromagnetic Curie-Weiss temperatures of 18.5 and 11.9 K, ordered ground states with net moments (low-moment ferromagnetism or canted antiferromagnetism), and zero field ordering temperatures of Tc= 6 K and Tc< 2 K, respectively. On the other hand, Na3Sc2Mo5O16 hosts a dynamical magnetic ground state with no evidence for magnetic ordering or spin freezing down to 20 mK despite an antiferromagnetic Curie-Weiss temperature of -36.2 K, and therefore is a candidate for quantum spin liquid behavior. By comparing the present results to past work on the same family of materials, we construct a phase diagram which illustrates that the magnetic ground states of these Mo-based molecular magnets are very sensitive to small changes in the nearest-neighbor Mo-Mo distance.

Original languageEnglish
Article number044414
JournalPhysical Review Materials
Volume6
Issue number4
DOIs
StatePublished - Apr 2022

Funding

We acknowledge valuable conversations with S. Streltsov and Y. B. Kim as well as technical support of the CMMS team at TRIUMF, in particular B. Hitti, G. Morris, D. Arseneau, and D. Vyas. Q.C., R.S., and H.D.Z. thank the support from Grant No. NSF-DMR-2003117. The work of Z.D. and M.M. at Georgia Tech was supported by Grant No. NSF-DMR-1750186. J.Q. and A.A.S. acknowledge funding from the Natural Sciences and Engineering Research Council of Canada and the Canada First Research Excellence Fund. A portion of this research used resources at the High Flux Isotope Reactor, which is a DOE Office of Science User Facility operated by Oak Ridge National Laboratory. A portion of this work was performed at the NHMFL, which is supported by National Science Foundation Cooperative Agreement No. DMR-1157490 and the state of Florida.

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