Abstract:The correlation of heating rates, crystal structures, and microwave dielectric properties of Li 2 ZnTi 3 O 8 ceramics was thoroughly investigated. Ionic polarizability, atomic packing fractions, bond strengths, and octahedral distortion of Li 2 ZnTi 3 O 8 ceramics were calculated on the basis of structure refinement data. The ''black core'' phenomenon resulting from reduction of Ti 4+ ions was observed for Li 2 ZnTi 3 O 8 ceramic sintered at 1°/min; reduction of Ti 4+ ions could be limited by heating more rapi… Show more
“…The binding energy of surface elements acquired from XPS could provide further information for structural change (Figure 8). In the survey spectra (Figure 8a), the C 1s peak (284.78 eV) is used as a reference for identifying other elements, besides the Li 1s, O 1s, Zn 2p, and Ti 2p peaks presented in P-LZTO and LZTO/KCl, 33 Cl 2p peak also displays in LZTO/KCl. The signal of K 2p could hardly be distinguished in the survey spectrum due to the less amount of K on the surface of LZTO particle and the overlap of K 2p peak (292.93 eV) with C 1s peak (284.78 eV) resulted from the similar binding energies of them, but could be revealed by the core level spectrum of K 2p (Figure 8e).…”
Inorganic salt of
KCl was first employed as an effective modifier
to modify Li2ZnTi3O8 anode material
via simply mixing in KCl solution followed by sintering at 800 °C
in air. The Li2ZnTi3O8 modified with
1.0 wt % KCl exhibited splendid rate capabilities (retaining reversible
capacities of 225.6, 195.4, 178.0, 162.4, and 135.6 mAh g–1 at 100, 200, 400, 800, and 1600 mA g–1, respectively)
and excellent long-term cycling stability (maintaining a capacity
of 201.6 mAh g–1 after 700 cycles). Combining structural
characterization with electrochemical analysis, the KCl modification
leads to simultaneous doping of K+ and Cl– in Li2ZnTi3O8, contributing to
enhance the electronic and ionic conductivities of Li2ZnTi3O8.
“…The binding energy of surface elements acquired from XPS could provide further information for structural change (Figure 8). In the survey spectra (Figure 8a), the C 1s peak (284.78 eV) is used as a reference for identifying other elements, besides the Li 1s, O 1s, Zn 2p, and Ti 2p peaks presented in P-LZTO and LZTO/KCl, 33 Cl 2p peak also displays in LZTO/KCl. The signal of K 2p could hardly be distinguished in the survey spectrum due to the less amount of K on the surface of LZTO particle and the overlap of K 2p peak (292.93 eV) with C 1s peak (284.78 eV) resulted from the similar binding energies of them, but could be revealed by the core level spectrum of K 2p (Figure 8e).…”
Inorganic salt of
KCl was first employed as an effective modifier
to modify Li2ZnTi3O8 anode material
via simply mixing in KCl solution followed by sintering at 800 °C
in air. The Li2ZnTi3O8 modified with
1.0 wt % KCl exhibited splendid rate capabilities (retaining reversible
capacities of 225.6, 195.4, 178.0, 162.4, and 135.6 mAh g–1 at 100, 200, 400, 800, and 1600 mA g–1, respectively)
and excellent long-term cycling stability (maintaining a capacity
of 201.6 mAh g–1 after 700 cycles). Combining structural
characterization with electrochemical analysis, the KCl modification
leads to simultaneous doping of K+ and Cl– in Li2ZnTi3O8, contributing to
enhance the electronic and ionic conductivities of Li2ZnTi3O8.
“…The enlarged (311) peak in Figure 1b reveals a slight shift to a lower angle in LZTO@RGO10 and LZTO@RGO25 owing to the creation of oxygen vacancies due to the incomplete crystallinity of LZTO in the presence of RGO. 40 This lattice property may be suitable for rapid transportation of Li + ions during the charge-discharge process. Due to the fact that LZTO@RGO composites have smaller crystalline size and larger lattice constants, we expect that Li + diffusion can be easier than that of the pristine LZTO anode.…”
Li 2 ZnTi 3 O 8 (LZTO) and reduced graphite oxide modified Li 2 ZnTi 3 O 8 which are designated as LZTO@RGO10, LZTO@RGO25 and LZTO@RGO50 anodes were successfully prepared by a facile and cost effective ball mill assisted solid state method. RGO/LZTO mass ratios were selected as 0.1: 1, 0.25:1 and 0.5:1, respectively. The effects of RGO content on the crystal lattice, particle morphology and electrochemical properties were investigated. The electrochemical performance of LZTO could be improved by adjusting the content of RGO. Among all the samples, LZTO@RGO25 exhibits excellent electrochemical performance in terms of high capacities (302, 250, 221, 194 and 154 mAh g −1 at current densities of 0.1, 0.5, 1, 2 and 5C, respectively). Cycling performance measurements show that , LZTO@RGO25 has 200 mAh g −1 residual capacity compared with that (66 mAh g −1 ) of LZTO after 100 cycles at 1C rate.
“…Except for the sintering temperature, the heating rates and substation will directly influence the grain size, densification, and properties. Lu et al [254] pointed out that the sintering rate increasing from 3 to 7 /min would deteriorate the quality f ℃ actor of Li 2 ZnTi 3 O 8 ceramics. If ball milling is applied for the raw materials at first for 4 h, then the sintering temperature of Li 2 ZnTi 3 O 8 ceramics could reduce from 1075 to 925 , and those ceramics were chemically ℃ compatible with Ag [255].…”
The explosive process of 5G communication evokes the urgent demand of miniaturized and integrated dielectric ceramics filter. It is a pressing need to advance the development of dielectric ceramics utilization of emerging technology to design new materials and understand the polarization mechanism. This review provides the summary of the study of microwave dielectric ceramics (MWDCs) sintered higher than 1000 from 2010 up to now, °C with the purpose of taking a broad and historical view of these ceramics and illustrating research directions. To date, researchers endeavor to explain the structure-property relationship of ceramics with multitude of approaches and design a new formula or strategy to obtain excellent microwave dielectric properties. There are variety of factors that impact the permittivity, dielectric loss, and temperature stability of dielectric materials, covering intrinsic and extrinsic factors. Many of these factors are often intertwined, which can complicate new dielectric material discovery and the mechanism investigation. Because of the various ceramics systems, pseudo phase diagram was used to classify the dielectric materials based on the composition. In this review, the ceramics were firstly divided into ternary systems, and then brief description of the experimental probes and complementary theoretical methods that have been used to discern the intrinsic polarization mechanisms and the origin of intrinsic loss was mentioned. Finally, some perspectives on the future outlook for high-temperature MWDCs were offered based on the synthesis method, characterization techniques, and significant theory developments.
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