Haizhou Guo

Haizhou Guo


Research Focus & Metrics

Academic Career Length

2Years (2025-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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23 April 2025 in Coatings
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Journal Article
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EWErping Wang
Erping Wang
HYHongjun Yang
Hongjun Yang
HGHaizhou Guo
Haizhou Guo
HLHongxia Li
Hongxia Li
HZHaosong Zhang
Haosong Zhang
YZyangyang Zhang
yangyang Zhang
Relaxor ferroelectrics based on sodium bismuth titanate (Bi0.5Na0.5TiO3, BNT) have attracted more interest recently as potential ecologically acceptable materials for pulse power technology because of their excellent full-energy storage capabilities. This paper formed (1 − x){0.97[0.98(BNT-ST)-0.02CN]-0.03AlN}-xNN ceramics through a traditional solid-state reaction process. It was noted that the incorporation of NaNbO3 enhances the property of energy storage by elevating the breakdown strength and causing the creation of an ergodic relaxation state. The effective energy storage density (Wrec) and the energy storage efficiency (η) are 1.09 J/cm3 and 85%, respectively. The breakdown field strength Eb reached 155 kV/cm at x = 40%. These ceramics have excellent temperatures and frequency stabilities from 0.5 to 50 Hz and 20 to 60 °C.

20 March 2025 in Crystals
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JGJingxia Gao
Jingxia Gao
HGHaizhou Guo
Haizhou Guo
HLHongxia Li
Hongxia Li
HLHui Li
Hui Li
LYLiqin Yue
Liqin Yue
YZyangyang Zhang
yangyang Zhang
Dielectric capacitors with a high density of recoverable energy storage are extremely desirable for a variety of uses. However, these capacitors often exhibit lower breakdown strengths and energy efficiency compared to other materials, which poses significant challenges for their practical use. We report on a novel antiferroelectric ceramic system in the present study, (1 − x){0.97[0.985(0.93Bi0.5Na0.5TiO3–0.07BaTiO3)–0.015Er)]–0.03AlN}–xNaNbO3 (x = 0, 10 wt%, 20 wt%, 30 wt%, and 40 wt%), synthesized via a conventional solid-state reaction approach. Here, (Bi0.5Na0.5TiO3–BaTiO3) is denoted as BNT–BT. We observed that varying the NaNbO3 (NN) content gradually refined the grain size of the ceramics, narrowed their hysteresis loops, and transformed their phase structure from antiferroelectric to relaxor ferroelectric. These changes enhanced breakdown strength (Eb), thus increasing the performance of energy storage. Specifically, the recoverable energy density (Wrec) and energy storage efficiency (η), respectively, reached 0.67–1.06 J/cm3 and 44–88% at electric fields of 110–155 kV/cm, with the highest performance observed at 30 wt% NN doping. Additionally, over a broad range of temperature and frequency, the 70 wt% {0.97[0.985(BNT–BT)–0.015Er]–0.03AlN}–30 wt% NN ceramic demonstrated exceptional stability in energy storage. These results demonstrate the significant potential of lead-free(1 − x)({0.97[0.985(BNT–BT)–0.015Er]–0.03AlN}–xNN ceramics for the applications of high-performance energy storage.

28 October 2025 in Materials
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Journal Article
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YZyangyang Zhang
yangyang Zhang
HGHaizhou Guo
Haizhou Guo
SZShuyao Zhai
Shuyao Zhai
LYLiqin Yue
Liqin Yue
JZJuqin Zhang
Juqin Zhang
LZLing Zhang
Ling Zhang
(Bi0.5Na0.5)TiO3-based lead-free ferroelectric ceramics are among the most extensively researched energy storage materials today. In this paper, (1 − x)Bi0.46Sr0.06Na0.5TiO3−xCaTiO3 ceramics were synthesized through a solid-phase sintering method by synergistically adjusting CaTiO3 components after introducing Sr2+ at the A-site. The XRD patterns revealed that all samples formed a single perovskite solid solution, with the 111 and 200 peaks shifting to higher levels as the CaTiO3 increased, indicating a gradual decrease in cell volume. The SEM images exhibited dense crystals without any apparent porosity, which were formed by the different components of the ceramics. Through energy storage, dielectric, and charge–discharge performance tests, it was found that with a 10%mol CaTiO3 addition, the samples obtained a maximum breakdown field strength of 260 kV/cm and corresponding saturation polarization strength of 32.80 μC/cm2 and thereby exhibited a reversible energy storage density valued 3.52 J/cm3. In addition, the dielectric constant varied by less than 10% within the temperature range of 63.7 °C to 132.7 °C and presented good frequency (10–250 Hz) stability at 180 kV/cm. Moreover, the ceramics demonstrated a maximum current density reaching 349.58 A/cm2 and a maximum power density of 18.90 MW/cm3 for their charge–discharge performance, all of which makes them suitable for pulse system applications.