Antiferromagnetism of Zn2VO(PO4)(2) and the dilution with Ti4+

Article

关键词: QUANTUM HEISENBERG-ANTIFERROMAGNET;    SPIN-LATTICE RELAXATION;    SQUARE-LATTICE;    CORRELATION LENGTH;    GROUND-STATE;    TEMPERATURE;    FERROMAGNETISM;    SYSTEMS;    MODEL;    NMR;   

DOI  :  10.1103/PhysRevB.91.024413

来源: SCIE

【 摘 要 】

We report static and dynamic properties of the antiferromagnetic compound Zn2VO(PO4)(2), and the consequences of nonmagnetic Ti(4+)doping at the V(4+)site. P-31 nuclear magnetic resonance (NMR) spectra and spin-lattice relaxation rate (1/T-1) consistently show the formation of the long-range antiferromagnetic order below T-N = 3.8-3.9 K. The critical exponent beta = 0.33 +/- 0.02 estimated from the temperature dependence of the sublattice magnetization measured by P-31 NMR at 9.4 MHz is consistent with universality classes of three-dimensional spin models. The isotropic and axial hyperfine couplings between the P-31 nuclei and V4+ spins are A(hf)(iso) = (9221 +/- 100) Oe/mu B and A(ax) (hf) = (1010 +/- 50) Oe/mu B, respectively. Magnetic susceptibility data above 6.5 K and heat capacity data above 4.5 K are well described by quantum Monte Carlo simulations for the Heisenberg model on the square latticewith J similar or equal to 7.7K. This value of J is consistent with the values obtained from the NMR shift, 1/T-1, and electron spin resonance intensity analysis. Doping Zn2VO(PO4)(2) with nonmagnetic Ti4+ leads to a marginal increase in the J value and the overall dilution of the spin lattice. In contrast to the recent ab initio results, we find neither evidence for the monoclinic structural distortion nor signatures of the magnetic one-dimensionality for doped samples with up to 15% of Ti4+. The Neel temperature T-N decreases linearly with increasing the amount of the nonmagnetic dopant.

【 授权许可】

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