Low frequency dielectric behavior and AC conductivity of polymer derived SiC(O)/HfCxN1-x ceramic nanocomposites

The dielectric behavior of spark plasma sintered SiC(O)/HfCxN1-x nanocomposites synthesized through polymer derived ceramic route was investigated in the frequency range of 1 kHz to 1 MHz at room temperature. The nanostructural features revealed HfCxN1-x nanocrystals encapsulated in a nanometric thi...

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Veröffentlicht in:Materials chemistry and physics 2021-02, Vol.260, p.124122, Article 124122
Hauptverfasser: Awin, Eranezhuth Wasan, Sridar, Soumya, Kousaalya, Adhimoolam Bakthavachalam, Vendra, S.S. Lokesh, Koroleva, Ekaterina, Filimonov, Alexey, Vakhrushev, Sergey, Kumar, Ravi
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Sprache:eng
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Zusammenfassung:The dielectric behavior of spark plasma sintered SiC(O)/HfCxN1-x nanocomposites synthesized through polymer derived ceramic route was investigated in the frequency range of 1 kHz to 1 MHz at room temperature. The nanostructural features revealed HfCxN1-x nanocrystals encapsulated in a nanometric thin layer of carbon dispersed uniformly in a SiC(O) matrix with segregated free carbon. The nanocomposites exhibited colossal permittivity values in the order of 103 at 1 kHz which reduced to 646 at 1 MHz. The interfacial polarization mechanism existing between complex nanostructural interfaces and the percolation of HfCxN1-x nanocrystals are believed to be responsible for the high permittivity values observed in the measured frequency range. The AC conductivity exemplified a frequency independent behavior at lower frequencies while at higher frequencies, the conductivity exhibited frequency dependence, indicating the existence of hopping type mechanism. [Display omitted] •In situ crystallization of size controlled SiC(O)/HfCxN1-x nanocrystals through PDC route.•Core-shell structure and presence of free carbon enhances the permittivity values.•Colossal high permittivity values due to the space charge polarization mechanism.•AC conductivity followed Jonscher’s law implying hopping type mechanism.
ISSN:0254-0584
1879-3312
DOI:10.1016/j.matchemphys.2020.124122