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Novel Temperature Stable Li_2MnO_3 Dielectric Ceramics with High Q for LTCC Applications

机译:用于LTCC应用的新型高Q温度稳定Li_2MnO_3介电陶瓷

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摘要

Novel microwave dielectric ceramics in the Li_2MnO_3 system with high Q prepared through a conventional solid-state route had been investigated. All the specimens exhibited single phase ceramics sintered in the temperature range 1140℃-1230℃. The microwave dielectric properties of Li_2MnO_3 ceramics were strongly correlated with sintering temperature and density. The best microwave dielectric properties of ε_r = 13.6, Q×f=97 000 (GHz), and τ_f= -5.2 ppm/℃ could be obtained as sintered at 1200℃ for 4 h. BaCu(B_2O_5) (BCB) could effectively lower the sintering temperature from 1200℃ to 930℃ and slightly induced degradation of the microwave dielectric properties. The Li_2MnO_3 ceramics doped with 2 wt % BaCu(B_2O_5) had excellent dielectric properties of ε_r = 11.9, Q׃= 80 600 (GHz), and τ_ƒ= 0 ppm/℃. With low sintering temperature and good dielectric properties, the BCB added Li_2MnO_3 ceramics are suitable candidates for LTCC applications in wireless communication system.
机译:研究了通过常规固态途径制备的高Q值的Li_2MnO_3体系中的新型微波介电陶瓷。所有样品均表现出在1140℃-1230℃温度范围内烧结的单相陶瓷。 Li_2MnO_3陶瓷的微波介电性能与烧结温度和密度密切相关。在1200℃烧结4 h可获得最佳的微波介电常数ε_r= 13.6,Q×f = 97 000(GHz)和τ_f= -5.2 ppm /℃。 BaCu(B_2O_5)(BCB)可以有效地将烧结温度从1200℃降低到930℃,并引起微波介电性能的轻微降低。掺杂有2 wt%BaCu(B_2O_5)的Li_2MnO_3陶瓷具有极好的介电性能,ε_r= 11.9,Q׃= 80 600(GHz),τ_ƒ= 0 ppm /℃。具有较低的烧结温度和良好的介电性能,BCB添加的Li_2MnO_3陶瓷是无线通信系统中LTCC应用的合适候选材料。

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  • 来源
    《Journal of the American Ceramic Society》 |2014年第6期|1918-1922|共5页
  • 作者单位

    Department of Electronic Engineering, National United University, No. 1 36003, Taiwan;

    Department of Electronic Engineering, National United University, No. 1 36003, Taiwan;

    Department of Electronic Engineering, National United University, No. 1 36003, Taiwan;

    Department of Electronic Engineering, National United University, No. 1 36003, Taiwan;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 eng
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  • 入库时间 2022-08-17 13:36:58

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