Bingfeng Ge, Jitao Zhang, Sujoy Saha, Sabita Acharya, Chaitrali Kshirsagar, Sidharth Menon, Menka Jain, Michael R. Page, G. Srinivasan
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For ME measurements, the fibers were pressed into disks and rectangular platelets and then annealed at 900–1000 °C for densification. The strengths of strain-mediated ME coupling were measured by the H-induced changes in remnant polarization Pr and by low-frequency ME voltage coefficient (MEVC). The fractional change in Pr under H increased in magnitude, from +3% for disks of NFO–PZT to −82% for NZFO (x = 0.3)-PZT, and a further increase in x resulted in a decrease to a value of −3% for x = 0.5. The low-frequency MEVC measured in disks of the core–shell fibers ranged from 6 mV/cm Oe to 37 mV/cm Oe. The fractional changes in Pr and the MEVC values were an order of magnitude higher than for bulk samples containing mixed fibers with a random distribution of NZFO and PZT. 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引用次数: 0
摘要
本报告研究的是带有镍锌铁氧体和 PZT 同轴纤维的块状复合材料中的磁电(ME)相互作用。采用电纺丝法制成了 PZT 和 Ni1-xZnxFe2O4 (NZFO)(x = 0-0.5)的核壳纤维。两种纤维的内核均为铁氧体或 PZT,直径在 1-3 μm 之间。电子显微镜和扫描探针显微镜图像显示,纤维成型良好,具有均匀的芯壳结构和无缺陷的界面。在 700-900 °C 下退火的纤维的 X 射线衍射数据未显示任何杂质相。磁化、磁致伸缩、铁磁共振和极化 P 与电场 E 的关系测量证实了纤维的铁性。为了进行 ME 测量,先将纤维压制成圆盘和矩形小板,然后在 900-1000 °C 下退火以进行致密化。应变介导的 ME 耦合强度是通过 H 诱导的残余极化 Pr 变化和低频 ME 电压系数(MEVC)测量的。H 下 Pr 的分数变化幅度增大,从 NFO-PZT 磁盘的 +3% 到 NZFO (x = 0.3)-PZT 的 -82%,x 的进一步增大导致 x = 0.5 时降至 -3%。在核壳纤维盘中测量到的低频 MEVC 范围为 6 mV/cm Oe 至 37 mV/cm Oe。与含有随机分布的 NZFO 和 PZT 混合纤维的块状样品相比,Pr 的分数变化和 MEVC 值要高出一个数量级。带有同轴纤维的块状复合材料有望用作磁场传感器和能量收集应用。
Evidence for a Giant Magneto-Electric Coupling in Bulk Composites with Coaxial Fibers of Nickel–Zinc Ferrite and PZT
This report is on magneto-electric (ME) interactions in bulk composites with coaxial fibers of nickel–zinc ferrite and PZT. The core–shell fibers of PZT and Ni1−xZnxFe2O4 (NZFO) with x = 0–0.5 were made by electrospinning. Both kinds of fibers, either with ferrite or PZT core and with diameters in the range of 1–3 μm were made. Electron and scanning probe microscopy images indicated well-formed fibers with uniform core and shell structures and defect-free interface. X-ray diffraction data for the fibers annealed at 700–900 °C did not show any impurity phases. Magnetization, magnetostriction, ferromagnetic resonance, and polarization P versus electric field E measurements confirmed the ferroic nature of the fibers. For ME measurements, the fibers were pressed into disks and rectangular platelets and then annealed at 900–1000 °C for densification. The strengths of strain-mediated ME coupling were measured by the H-induced changes in remnant polarization Pr and by low-frequency ME voltage coefficient (MEVC). The fractional change in Pr under H increased in magnitude, from +3% for disks of NFO–PZT to −82% for NZFO (x = 0.3)-PZT, and a further increase in x resulted in a decrease to a value of −3% for x = 0.5. The low-frequency MEVC measured in disks of the core–shell fibers ranged from 6 mV/cm Oe to 37 mV/cm Oe. The fractional changes in Pr and the MEVC values were an order of magnitude higher than for bulk samples containing mixed fibers with a random distribution of NZFO and PZT. The bulk composites with coaxial fibers have the potential for use as magnetic field sensors and in energy-harvesting applications.