Dimethylammonium copper formate [(CH3)2NH2]Cu(HCOO)3: A metal-organic framework with quasi-one-dimensional antiferromagnetism and magnetostriction

Zhenxing Wang, Prashant Jain, Kwang-Yong Choi, Johan van Tol, Anthony K. Cheetham, Harold W. Kroto, Hyun-Joo Koo, Haidong Zhou, Jungmin Hwang, Eun Sang Choi, Myung-Hwan Whangbo, and Naresh S. Dalal
Phys. Rev. B 87, 224406 – Published 10 June 2013

Abstract

Metal-organic frameworks (MOFs) can exhibit many interesting properties such as multiferroic behavior, dipolar glass, gas storage, and protonic conductivity. Here we report that dimethylammonium copper formate (DMACuF) [(CH3)2NH2]Cu(HCOO)3, a cation templated nonporous MOF with perovskite topology, exhibits strong one-dimensional (1D) antiferromagnetism with a Néel temperature, TN, of 5.2 K. These conclusions are derived from detailed magnetic susceptibility, heat capacity, dielectric constant, and high-frequency electron paramagnetic resonance measurements as well as density functional theory (DFT) calculations. The magnetic susceptibility exhibits a broad maximum at ∼50 K, suggesting low-dimensional magnetism; heat capacity measurements show a Néel temperature of 5.2 K. The magnetization versus field data at 1.8 K shows a spin-flop transition at Hsf ∼ 1.7 T. The ratio TN/J=6.5×102, where J is the near-neighbor exchange constant (77.4 K), and the small value (2 K) of the interchain coupling suggests that DMACuF is close to an ideal 1D magnet. In this three-dimensional crystal lattice, the 1D magnetic behavior is made possible by the Jahn-Teller distortion of the 3d9 Cu2+ ions. Temperature dependence of the electron paramagnetic resonance field and the linewidth exhibits critical broadening for temperatures below 50 K, following a behavior quite characteristic of 1D spin systems. DFT calculations show that [(CH3)2NH2]Cu(HCOO)3 has a magnetic structure in which 1D antiferromagnetic chains parallel to the c direction are weakly coupled ferromagnetically, supporting the thermomagnetic and EPR results. Dielectric measurements under applied magnetic fields of 0−7 T reveal a kink at the TN, a clear indication of magnetostriction behavior.

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  • Received 25 July 2012

DOI:https://doi.org/10.1103/PhysRevB.87.224406

©2013 American Physical Society

Authors & Affiliations

Zhenxing Wang1,2, Prashant Jain3,*, Kwang-Yong Choi4, Johan van Tol1,2, Anthony K. Cheetham5, Harold W. Kroto1, Hyun-Joo Koo6, Haidong Zhou2, Jungmin Hwang2,7, Eun Sang Choi2, Myung-Hwan Whangbo8, and Naresh S. Dalal1,2,†

  • 1Department of Chemistry and Biochemistry, Florida State University, Tallahassee, Florida 32306, USA
  • 2National High Magnetic Field Laboratory, Florida State University, Tallahassee, Florida 32310, USA
  • 3LANSCE-LC & NHMFL-PFF, Los Alamos National Laboratory, Los Alamos, New Mexico 87544, USA
  • 4Department of Physics, Chung-Ang University, 221 Huksuk-Dong, Dongjak-Gu, Seoul 156-756, Republic of Korea
  • 5Department of Materials Science and Metallurgy, University of Cambridge, Cambridge CB2 3QZ, United Kingdom
  • 6Department of Chemistry and Research Institute for Basic Sciences, Kyung Hee University, Seoul 130-701, Republic of Korea
  • 7Department of Physics, Florida State University, Tallahassee, Florida 32306, USA
  • 8Department of Chemistry, North Carolina State University, Raleigh, North Carolina 27695, USA

  • *Corresponding author: prashant@lanl.gov
  • Corresponding author: dalal@chem.fsu.edu

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Vol. 87, Iss. 22 — 1 June 2013

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