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Ceramics

Ceramics is an international, peer-reviewed, open access journal of ceramics science and engineering, published monthly online by MDPI.

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All Articles (812)

  • Article
  • Open Access

Phosphate glasses with the compositions 60P2O5–15ZnO–15CaO–10Li2O (PZCL) and 60P2O5–15ZnO–15CaO–10V2O5 (PZCV) (mol%, expressed as oxides) were synthesized by the melt-quenching method. The prepared glasses were characterized by using X-ray powder diffraction (XRD), Raman spectroscopy, scanning electron microscopy (SEM) and electrochemical impedance spectroscopy (EIS). X-ray diffraction shows only broad diffuse halos without Bragg reflections, indicating that both glasses are X-ray amorphous. Raman analysis confirms that PZCL behaves as a typical alkali-modified ultraphosphate glass containing Q3 and Q2 units, whereas PZCV contains characteristic V–O vibrational modes indicating that vanadate groups are integrated into the phosphate backbone. SEM observations reveal smooth surfaces at low magnification for both glasses; at higher magnification, PZCV shows a compact and homogeneous surface with fine, uniformly dispersed granules, whereas PZCL displays a more textured surface with agglomerates and plate-like features. EIS analysis using the Havriliak–Negami model reveals that the free-charge carrier contribution appears as a step in M′(ω,T) and a peak in M″(ω,T), allowing a clear distinction between conductivity relaxation and interfacial polarization or dipolar effects, with conductivity derived from the M″(ω,T) peak frequency. PZCV shows dc conductivity approximately one order of magnitude higher than PZCL (1.5 × 10−9 vs. 1.8 × 10−10 S·cm−1 at 120 °C). The temperature dependence follows Arrhenius behavior, with activation energies of about 0.89 eV for PZCV and 1.04 eV for PZCL. The electrode polarization observed at low frequencies with ion-blocking gold electrodes indicates a significant ionic contribution in both glasses, although a polaronic (V4+/V5+) contribution to the conductivity of PZCV cannot be excluded. Capacitance analysis reveals a slight increase with temperature for both samples, with PZCV consistently showing higher values (~7 pF) than PZCL (~5 pF). Although the absolute conductivities remain far below those required for practical solid electrolytes, these results clarify how the replacement of Li2O by V2O5 modifies charge transport and dielectric relaxation in P2O5-rich Zn–Ca phosphate glasses.

Ceramics

5 November 2026

X-ray diffraction patterns of PZCV (a) and PZCL (b).
  • Article
  • Open Access

Multiphasic calcium phosphate (CaP) composites made of hydroxyapatite (HAp), α-tricalcium phosphate (α-TCP), or β-tricalcium phosphate (β-TCP) are promising for biomedical applications. In this paper, the changes in Raman spectra of a series of HAp/α-TCP and HAp/β-TCP were calibrated and new algorithms using microRaman spectroscopy were established for an efficient and quantitative analysis of the constituent phases in multiphasic CaP systems, taking advantages of their characteristic Raman bands. The reliability of the proposed Raman algorithms was further examined and verified by the investigation of a tri-phase CaP mixture and thermally treated monolithic ceramics of HAp, α-TCP and β-TCP using both Raman and XRD analyses. The results demonstrated the applicability of the proposed method for quantitative phase evaluation, as well as higher sensitivity of Raman spectroscopy to nonstoichiometric alteration for more precise phase control and quality evaluation in the presence of defects in multiphasic CaP systems.

Ceramics

3 November 2026

(a) Representative Raman spectra of α-TCP, β-TCP, and hydroxyapatite, and (b) respective ν1 band in the enlarged spectral region of 920–1000 cm−1.
  • Article
  • Open Access

Lead-free (1−x)(K0.49Na0.51)(Nb0.95Sb0.05)O3-xSr(Fe0.5Nb0.5)O3 [(1−x)KNNbS-xSrFNb, x = 0.01–0.07] ceramics with 0.5 wt% CuO were prepared by conventional sintering (CS) and two-step sintering (TSS). Increasing the SrFNb content drives the structure from orthorhombic–tetragonal (O-T, x ≤ 0.03) coexistence to rhombohedral–tetragonal (R-T, x ≥ 0.05) coexistence, and shifts the phase boundary toward room temperature, while Fe3+/Nb5+ B-site disorder induces polar nanoregions, diffuse dielectric behavior (dispersion index γ > 1.7) and a drop of Tm (temperature of dielectric constant maximum) from 295 °C to below room temperature. Increasing SrFNb significantly reduces the average grain size from 0.6 μm to 0.3 μm, while TSS decouples densification from grain growth, raising the maximum relative density from 92.13% to 94.51% at x = 0.05 with only a slight reduction in average grain size from 0.35 μm to 0.32 μm. These changes directly tailor the electrical properties: the near-room-temperature O-T boundary at x = 0.03 gives the best soft-type response (piezoelectric constant d33 = 133 pC/N, electromechanical coupling coefficient Kp = 0.285, remnant polarization Pr = 22.72 μC/cm2), whereas acceptor-oxygen-vacancy dipoles at x = 0.01 pin domain walls, yielding the highest mechanical quality factor Qm = 329 with low tan δ, and TSS further improves fatigue resistance. Combining SrFNb-driven structural evolution with TSS microstructural control thus offers an effective route to tailor KNN-based lead-free piezoelectrics.

Ceramics

31 October 2026

XRD patterns of (a) the 0.95KNNbS-0.05SrFNb ceramics sintered by CS and TSS at different temperatures, and (b) the (1−x)KNNbS-xSrFNb ceramics with different SrFNb doping contents prepared by TSS and (c) their zoom-in XRD patterns around the (200) peak.
  • Article
  • Open Access

This work elucidates the growth of lithium nickel cobalt manganese oxide (NCM)/lithium lanthanum zirconate (LLZO)/zinc ferrite (ZFO) films using X-ray diffraction (XRD), Rutherford backscattering (RBS), electron probe microanalysis (EPMA) and X-ray absorption spectroscopy (XAS). Prior to deposition of LLZO and NCM/LLZO, ZFO films (deposition times: 25 (NLZ25) and 100 min (NLZ100)) were deposited on silicon (100) substrates using radio frequency (RF) sputtering at a base pressure of 5.0 × 10−6 Torr. LLZO was deposited for 90 min at RF power of 40 W. Thereafter, an NCM layer was deposited on these bilayer structures for 100 min (RF power—35 W). Obtained trilayer structures were annealed at 900 °C for 1 h. XRD shows ZFO is able to attain crystalline phase of spinel structure for both NLZ25 and NLZ100. In the trilayer structures onsets of some impurity phases are observed. RBS analysis reveals that for NLZ25, NCM, LLZO, and ZFO layers have thicknesses of approximately 30, 60, and 70 nm. For NLZ100, the corresponding layer thicknesses are 40, 90, and 200 nm, respectively. The significant change in ZFO thickness is attributed to the longer deposition duration for later cases. The O K-edge near-edge X-ray absorption fine structure (NEXAFS) spectra of grown trilayer structures exhibit spectral features associated with ZFO, LLZO and NCM. The pre-edge region in the O K-edge NEXAFS spectra is strongly influenced by the interaction of ions from various layers in these structures. La M-edge NEXAFS spectra exhibit characteristic spectral features of La ions in LLZO and show the presence of La3+ in respective layers.

Ceramics

31 October 2026

Schematic of a thin-film battery showing various components and its approximate thickness.

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Ceramics - ISSN 2571-6131