4.6 Article

Deformed spin-1/2 square lattice in antiferromagnetic NaZnVOPO4(HPO4)

Journal

PHYSICAL REVIEW B
Volume 106, Issue 2, Pages -

Publisher

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevB.106.024426

Keywords

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Funding

  1. SERB, India [CRG/2019/000960]
  2. Prime Ministers Research Fellowship (PMRF) scheme, Government of India
  3. HLD at HZDR
  4. U.S. Department of Energy, Office of Science, Basic Energy Sciences, Materials Sciences and Engineering Division
  5. U.S. Department of Energy by Iowa State University [DEAC02-07CH11358]

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The structural and magnetic properties of a new spin-1/2 antiferromagnet NaZnVOPO4(HPO4) were studied using various methods, revealing significant magnetic behaviors and characteristics. The findings suggest that this compound exhibits unique features that deviate from conventional models.
We report the structural and magnetic properties of a new spin-1/2 antiferromagnet NaZnVOPO4(HPO4) studied via x-ray diffraction, magnetic susceptibility, high-field magnetization, specific heat, and P-31 nuclear magnetic resonance (NMR) measurements, as well as density-functional band-structure calculations. While thermodynamic properties of this compound are well described by the J(1)-J(2) square-lattice model, ab initio calculations suggest a significant deformation of the spin lattice. From fits to the magnetic susceptibility we determine the averaged nearest-neighbor and second-neighbor exchange couplings of J(1) similar or equal to -1.3K and J(2) similar or equal to 5.6K, respectively, resulting in the effective frustration ratio alpha = J(2)/J(1) similar or equal to -4.3 that implies columnar antiferromagnetic order as the ground state. Experimental saturation field of 15.3 T is consistent with these estimates if 20% spatial anisotropy in J(1) is taken into account. Specific heat data signal the onset of a magnetic long-range order at T-N similar or equal to 2.1K, which is further supported by a sharp peak in the NMR spin-lattice relaxation rate. The NMR spectra mark the superposition of two P lines due to two nonequivalent P sites where the broad line with the strong hyperfine coupling and short T-1 is identified as the P(1) site located within the magnetic planes, while the narrow line with the weak hyperfine coupling and long T-1 is designated as the P(2) site located between the planes.

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