2018
DOI: 10.1016/j.jeurceramsoc.2017.08.040
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(Al3+, Nb5+) co–doped CaCu3Ti4O12: An extended approach for acceptor–donor heteroatomic substitutions to achieve high–performance giant–dielectric permittivity

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Cited by 74 publications
(65 citation statements)
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“…Recently, giant dielectric materials belonging to the family of ACu 3 Ti 4 O 12 compounds have generated considerable interest due to their potential applications for the miniaturization of microelectronic devices, for example, multilayer ceramic capacitors. CaCu 3 Ti 4 O 12 (CCTO) is a popular material among the ACu 3 Ti 4 O 12 compounds because it exhibits a very large dielectric permittivity ( ε ′ ~10 4 ) over a wide temperature range without a detectable phase transition in the temperature range of 35‐100 K . However, a structural phase transition occurred in CCTO ceramics at 726‐732 K .…”
Section: Introductionmentioning
confidence: 99%
“…Recently, giant dielectric materials belonging to the family of ACu 3 Ti 4 O 12 compounds have generated considerable interest due to their potential applications for the miniaturization of microelectronic devices, for example, multilayer ceramic capacitors. CaCu 3 Ti 4 O 12 (CCTO) is a popular material among the ACu 3 Ti 4 O 12 compounds because it exhibits a very large dielectric permittivity ( ε ′ ~10 4 ) over a wide temperature range without a detectable phase transition in the temperature range of 35‐100 K . However, a structural phase transition occurred in CCTO ceramics at 726‐732 K .…”
Section: Introductionmentioning
confidence: 99%
“…The obtained parameters from general structure analysis system​ (GSAS) refinement fitting are displayed in Table . Our refinement achieved a good reliability . It was observed that the obtained lattice parameter ( a / b / c ) values for CdCTO‐04Zn and CdCTO‐08Zn are not significantly different from those for CdCTO, which probably results from the very similar ionic radii of Zn 2+ (0.60 Å) and Cu 2+ ions (0.57 Å).…”
Section: Resultsmentioning
confidence: 56%
“…The dielectric permittivity maintains a high value above 2.0 × 10 4 and seems to be frequency independent when the measured frequency is below 10 5 Hz, while a sharp decrease to ~100 occurs when the frequency reaches 10 7 ~10 8 Hz. This is a typical characteristic of the Debye (Maxwell‐Wagner) frequency response, and the dielectric plateau at low frequencies could be attributed to the electronic heterogeneity in the CdCu 3− x Zn x Ti 4 O 12 ceramics . To better understand the effect of Zn doping, we display the dielectric permittivity and dielectric loss tangent as a function of the Zn contents at 0.1, 1, and 10 kHz in Figure B.…”
Section: Resultsmentioning
confidence: 99%
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