Effect of Molybdenum Incorporation on the Structure and Magnetic Properties of Cobalt Ferrite

Journal Article · Tue Sep 26 00:00:00 EDT 2017 · Journal of Physical Chemistry. C

DOI:https://doi.org/10.1021/acs.jpcc.7b08162· OSTI ID:1410340

Orozco, C. ^[1]; Melendez, A. ^[1]; Manadhar, S. ^[1]; Singamaneni, S. R. ^[1]; Reddy, Kongara M. ^[2]; Gandha, K. ^[3]; Niebedim, I. C. ^[3]; Ramana, C. V. ^[1]

---

1. Univ. of Texas at El Paso, El Paso, TX (United States)
2. Boise State Univ., Boise, ID (United States)
3. Ames Lab., Ames, IA (United States)

Here, we report on the effect of molybdenum (Mo) incorporation on the crystal structure, surface morphology, Mo chemical valence state, and magnetic properties of cobalt ferrite (CoFe₂O₄, referred to CFO). Molybdenum incorporated cobalt ferrite (CoFe_2–xMo_xO₄, referred to CFMO) ceramics were prepared by the conventional solid-state reaction method by varying the Mo concentration in the range of x = 0.0–0.3. X-ray diffraction studies indicate that the CFMO materials crystallize in inverse spinel cubic phase. Molybdenum incorporation induced lattice parameter increase from 8.322 to 8.343 Å coupled with a significant increase in density from 5.4 to 5.7 g/cm³ was evident in structural analyses. Scanning electron microscopy imaging analyses indicate that the Mo incorporation induces agglomeration of particles leading to larger particle size with increasing x(Mo) values. Detailed X-ray photoelectron spectroscopic (XPS) analyses indicate the increasing Mo content with increasing x from 0.0 to 0.3. XPS confirms that the chemistry of Mo is complex in these CFMO compounds; Mo ions exist in the lower oxidation state (Mo⁴⁺) for higher x while in a mixed chemical valence state (Mo⁴⁺, Mo⁵⁺, Mo⁶⁺) for lower x values. From the temperature-dependent magnetization, the samples show ferrimagnetic behavior including the pristine CFO. From the isothermal magnetization measurements, we find almost 2-fold decrease in coercive field (H_c) from 2143 to 1145 Oe with the increase in Mo doping up to 30%. This doping-dependent H_c is consistently observed at all the temperatures measured (4, 100, 200, and 300 K). Furthermore, the saturation magnetization estimated at 4 K and at 1.5 T (from M–H loops) goes through a peak at 92 emu/g (at 15% Mo doping) from 81 emu/g (pristine CFO), and starts decreasing to 79 emu/g (at 30% Mo doping). The results demonstrate that the crystal structure, microstructure, and magnetic properties can be tuned by controlling the Mo-content in the CFMO materials.

• Research Organization: Ames Lab., Ames, IA (United States)
• Sponsoring Organization: USDOE
• Grant/Contract Number: AC02-07CH11358
• OSTI ID: 1410340
• Report Number(s): IS-J-9501
• Journal Information: Journal of Physical Chemistry. C, Vol. 121, Issue 45; ISSN 1932-7447
• Publisher: American Chemical Society
• Country of Publication: United States
• Language: English

Related Subjects

37 INORGANIC, ORGANIC, PHYSICAL, AND ANALYTICAL CHEMISTRY
36 MATERIALS SCIENCE