Olivine-type A2BO4 ceramics possess a low permittivity (εr) and low dielectric loss, contributing to a high quality factor (Q×f). However, the large negative temperature coefficient of the resonant frequency (τf) restricts their practical applications. In this work, we prepared a series of CaYGa1−xAlxO4 (x = 0–1) ceramics with low εr values via solid-state sintering. By controlling the evolution of orthorhombic olivine to the tetragonal perovskite-like structure (K2NiF4) and the ordered regulation of the A-site, an ultralow loss (tanδ = 1.38×10−4, Q×f = 125,530 GHz, and f = 17.3 GHz for x = 0) and a nearly zero temperature coefficient (τf = −0.5 ppm/°C for x = 0.9) were achieved. The significant changes in the dielectric properties (εr = 8.3–16.2, Q×f = 125,530–50,660 GHz, and τf = −50.9 to 2.9 ppm/°C) of these ceramics are primarily influenced by the characteristics of the second phase, ion polarization, ion order and disorder, and the chemical bonds resulting from structural evolution. Furthermore, a cylindrical dielectric resonator antenna (CDRA) was designed using an ultralow-loss CaYGaO4 ceramic, achieving a high gain (5.36–6.15 dBi) and efficiency (> 90%) in the bandwidth region (5.065–5.747 GHz), thereby enhancing the efficiency and quality of 5G communications. This work advances the development of control strategies for high-performance dielectric ceramics and dielectric resonator antennas in high-frequency communications.
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Open Access
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The low dielectric constant (εr < 15) is the key to improving the signal transmission speed of microwave communication devices. However, the resonant frequency temperature coefficient (τf) of most low-εr microwave dielectric ceramics is usually negative. Aiming to modify the large negative τf of scheelite CaWO4 and explore the underlying mechanism between the structure and microwave dielectric properties, a series of Ca1–x(Li1/2Eu1/2)xWO4 (x = 0.1−1.0) (CLEWOx) ceramics were prepared at low sintering temperatures (750−875 ℃). The εr increased from 10.46 to 18.55, and the Q× f decreased from 39,032 GHz–7425 GHz, mainly due to the enhanced rattling effect of Li+. The τf rapidly increased from negative (−19.91 × 10−6 ℃−1) to abnormally positive (+162.15 × 10−6 ℃−1), influenced by the reduced temperature coefficient of ion polarizability (ταm) caused by the rattling Li + cation. The CLEWO0.15 sample has good comprehensive performance (εr = 12.28, Q×f = 28,027 GHz, and τf = −0.5 × 10−6 ℃−1) and compatibility with the Ag electrode, showing the potential of LTCC applications. Additionally, a dielectric resonator antenna based on CLEWO0.15 ceramic was designed with a bandwidth of 254 MHz at 4.504−4.758 GHz and a gain of 4.87 dBi at 4.62 GHz, indicating that CLEWO0.15 may be a potential candidate for dielectric resonator antennas.
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Zircon ceramics have potential applications in next-generation wireless communication because of their low permittivity and adjustable temperature coefficient at microwave frequencies. However, the vast challenge of realizing ultralow dielectric loss still exists. Here, we propose a high-entropy strategy to enhance the bonding of the A-site dodecahedron in zircon and design (Nd0.2Eu0.2Y0.2Ho0.2Yb0.2)VO4 ceramics with a high quality factor (high Q × f, that is, low dielectric loss). The (Nd0.2Eu0.2Y0.2Ho0.2Yb0.2)VO4 high-entropy ceramics, which belong to the tetragonal zircon structure with the I41/amd space group, exhibit a low relative permittivity (εr = 11.55), a negative temperature coefficient of resonant frequency (τf = −37.3 ppm/°C), and a high Q × f of 76,400 GHz (at 12.31 GHz). The high Q × f value can be attributed to the high chemical bond strength and structural stability. Furthermore, the relationship between the crystal structure and the microwave dielectric properties of (Nd0.2Eu0.2Y0.2Ho0.2Yb0.2)VO4 high-entropy ceramics was analyzed through high resolution transmission electron microscopy (HRTEM), Raman spectroscopy, far-infrared reflection spectroscopy, and chemical bond theory. This work provides an effective avenue for designing microwave dielectric materials with low loss to meet the demands of passive components.
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