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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, and H. D. Zhou
Phys. Rev. Materials 6, 044414 – Published 28 April 2022

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.

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  • Received 4 March 2022
  • Accepted 5 April 2022

DOI:https://doi.org/10.1103/PhysRevMaterials.6.044414

©2022 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Q. Chen1, R. Sinclair1, A. Akbari-Sharbaf2, Q. Huang1, Z. Dun3, E. S. Choi4, M. Mourigal3, A. Verrier2, R. Rouane2, X. Bazier-Matte2, J. A. Quilliam2,*, A. A. Aczel5,†, and H. D. Zhou1,‡

  • 1Department of Physics and Astronomy, University of Tennessee, Knoxville, Tennessee 37996-1200, USA
  • 2Institut Quantique and Département de Physique, Université de Sherbrooke, 2500 boul. de l'Université, Sherbrooke, Québec, Canada J1K 2R1
  • 3School of Physics, Georgia Institute of Technology, Atlanta, Georgia 30332, USA
  • 4High Magnetic Field Laboratory, Florida State University, Tallahassee, Florida 32306-4005, USA
  • 5Neutron Scattering Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA

  • *jeffrey.quilliam@usherbrooke.ca
  • aczelaa@ornl.gov
  • hzhou10@utk.edu

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Vol. 6, Iss. 4 — April 2022

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