| The hexaferrite is an important material which is widely used in microwave processing, and how to regulate the saturation magnetization and the coercivity of the hexaferrite in large range is a significant research topic in preparing this microwave processing materials, In this paper, spark plasma sintering (SPS) technique was used to synthesize a series of M-type, W-type and Z-type barium ferrites induced multiphase ferrite mateials in large range to regulate saturation magnetizations and coercivities with metal iron as an induced agent. The phase composition, crystallization reaction mechanism, microsturcture and magnetic properties of the multiphase ferrite materials were comprehensively studied.By regulating the SPS sintering temperature, holding time and pressure, the optimized condition is holding 30 min at 900℃and 20 MPa for synthesizing M-type barium ferrite (BaM) induced multiphase ferrite materials. M-type barium ferrite induced multiphase ferrite materials were synthesized by sintering the coprecipitation precursors with nominal composition of xFe + BaFe12O19(0≤x≤1,△x=0.1) under the optimized SPS condition. The multiphase ferrite mat1erials were composed of BaM, Fe3O4 and Ba2Fe14O22 (Fe2Y) for 03 and Fe(OH)3 to form BaM, Fe(OH)3 and Fe to form Fe3O4, BaM and Fe3O4 to form Fe2Y; the multiphase ferrite materials were composed of Fe3O4 and Fe2Y for 0.8≤x≤1.0, and the crystallization reaction is BaCO3, Fe(OH)3 and Fe to form Fe2Y and Fe3O4. Needle Fe2Y mainly occurred in the interface area between Fe3O4 and BaM. As the x increased, the saturation magnetization of the multiphase ferrite first reduced significantly and remained almost constant, finally remarkably decreased again and then slightly increased, the coercivity of the multiphase ferrite first increased significantly and then decreased slightly.A series of M-type, W-type and Z-type barium ferrite induced multiphase ferrite materials fabricated by sintering the mixtures of irons and single phase BaM, BaCo2Fe16O27 (Co2W) and Ba3Co2Fe24O41 (Co2Z) powders with nominal composition of xFe+BaFe12O19, xFe + BaCo2Fe16O27 and xFe + Ba3Co2Fe24O41 (0≤x≤1,△x=0.1) using SPS method at 900℃and 20 MPa holding for 30 min, respectively. To the M-type barium ferrite induced multiphase ferrite materials, the grain size, the saturation magnetization and the coercivity reduced gradually, but the density increased with the x increasing. The crystallization reaction is BaM and Fe to form Fe2Y and Fe3O4, when multiphase ferrite materials were composed of BaM, Fe3O4 and Fe2Y; the crystallization reaction are BaM and Fe to form Fe2Y and Fe3O4, Fe and Fe2Y to form BaFe2O4 and Fe3O4, when the multiphase ferrite materials were composed of Fe3O4, Fe2Y and BaFe2O4. To the W-type barium ferrite induced multiphase ferrite materials, the density increased, the saturation magnetization reduced and the coercivity increased and then reduced with the x increasing. The crystallization reaction is Co2W and Fe to form Ba2Co2Fe12O22(Co2Y), CoFe2O4 and Fe3O4 when multiphase ferrite materials were composed of Co2W, Fe3O4, Co2Y and CoFe2O4; the crystallization reaction are Co2W and Fe to form Co2Y, CoFe2O4 and Fe3O4, Fe and Co2Y to form BaFe2O4, Fe3O4 and CoFe2O4 when the multiphase ferrite materials were composed of Fe3O4, Co2Y, BaFe2O4 and CoFe2O4. To the Z-type barium ferrite induced multiphase ferrite materials, the density and the coercivity increased but the saturation magnetization reduced with the x increasing. The multiphase ferrite materials were composed of Co2Z, Fe3O4, BaFe2O4 and Co2Y, the Co2Z disappeared with x=1.0. The crystallization reaction mechanism is Co2Z and Fe to form Co2Y, Fe3O4 and BaFe2O4. |