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Electronic, magnetic and spectroscopic properties of doped Mn (1− x ) A x WO 4 ( A = Co, Cu, Ni and Fe) multiferroic: an experimental and DFT study

材料科学 兴奋剂 结晶学 物理 凝聚态物理 化学
作者
Priyanath Mal,Ganesh Bera,Pachineela Rambabu,Goverdhan Reddy Turpu,Brahmananda Chakraborty,Lavanya M. Ramaniah,Ravi Prakash Singh,Pintu Sen,Pradip Das
出处
期刊:Journal of Physics: Condensed Matter [IOP Publishing]
卷期号:29 (7): 075901-075901 被引量:25
标识
DOI:10.1088/1361-648x/aa4e64
摘要

Abstract The influence of dopants (Co, Cu, Fe and Ni) on the optical, electronic and magnetic properties of multiferroic MnWO 4 was studied using Raman spectroscopy, ultraviolet–visible spectroscopy (UV–Vis), magnetization measurements and density functional theory (DFT) calculations. The evolution of Raman spectra with different elemental substitutions at the Mn site was also studied, where the peak width increased with doping of higher mass elements (Co, Cu, Fe and Ni). UV–Vis diffuse reflectance spectroscopy on polycrystalline Mn (1− x ) A x WO 4 ( A = Co, Cu, Fe and Ni) (0 ⩽ x ⩽ 0. was performed. The evaluated electronic band gap decreasing with successive Co, Cu and Fe doping reflected the lower ionic radius of the substituted element, and for Ni-doped MnWO 4 the band gap increased slightly compared to the parent MnWO 4 . Bader charge transfer and a partial density of states (PDOS) analysis from DFT simulations predict the appearance of impurity states in the band gap region (of pure MnWO 4 ) from the d orbital of the dopant (Co, Cu and Fe) hybridized with the p orbital of the bonded O atoms due to charge transfer from O to the dopant, and reduced the band gap of Co, Cu and Fe-doped MnWO 4 . On the other hand, for Ni-doped MnWO 4 strong W–O hybridization occurring due to large charge transfer from oxygen to tungsten leads to an increase in the band gap. The band gap, computed using the GGA + U method, is close to the experimental value. The signature of the d–d transition observed in the UV spectra is explained in terms of the crystal field stabilization energy caused by the octahedral distortion present in the lattice. Three different antiferromagnetic phases (AF1, AF2 and AF3) are identified in MnWO 4 and also for the Co (18.75%)-doped sample. For Cu-doped samples, suppression of the AF1 phase and stabilization of the AF2 phase is observed up to 2 K. Successive doping of Cu leads to the diminution of magnetic frustration. A new magnetic order is identified for Ni-doped MnWO 4 in the temperature range 13.7–20 K.
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