Hongmei Jing, Shibo Zhao, Ting Wang, Wanbiao Hu, Liming Diwu, Jingru Xu, Peiqiao Han, Miao Liu, Zhuo Wang and Zixiong Sun
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In this work, we grew 0.75Ba<small><sub>0.15</sub></small>Ca<small><sub>0.85</sub></small>Zr<small><sub>0.1</sub></small>Ti<small><sub>0.9</sub></small>O<small><sub>3</sub></small>–0.15Bi(Zn<small><sub>2/3</sub></small>Ta<small><sub>1/3</sub></small>)O<small><sub>3</sub></small> (BCZT–BZT) thin films on 100 nm SrRuO<small><sub>3</sub></small>(SRO)-coated (001)-STO substrates at various deposition temperatures. Due to lattice mismatch, all films consist of a strained layer and a relaxed layer, with varying proportions, and the strained layer is considered to degrade the voltage endurance of the thin films. The <em>J</em>–<em>E</em> curve results indicate a conduction mechanism transition from Schottky emission to Ohmic contact, with the formation of a depletion layer, which is higher in resistivity, at the bottom of BCZT–BZT60 and BCZT–BZT65. Considering a phase evolution from T-phase to O-phase from the bottom up, directly observed in the TEM images, electric field redistribution with voltage endurance was thought to occur in these two thin films, which is confirmed by the mathematical derivation. The synergistic effects of the variation between the strained and relaxed layers, along with the transitions in the conduction mechanism, result in BCZT–BZT65 achieving the highest breakdown strength (<em>E</em><small><sub>b</sub></small>) of 7.01 MV cm<small><sup>−1</sup></small> and a recoverable energy density (<em>W</em><small><sub>rec</sub></small>) of 101.79 J cm<small><sup>−3</sup></small>. 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引用次数: 0
摘要
在取代传统内燃机方面,介质电容器被认为优于锂离子电池,因为它们没有充电时间长的缺点。与块状陶瓷和柔性复合薄膜的材料状态相比,薄膜形式的介电电容器在域和界面工程以外的调节方面具有更大的灵活性。在这项工作中,我们在 100 nm SrRuO3(SRO)涂层 (001)-STO 基底上,在不同沉积温度下生长了 0.75Ba0.15Ca0.85Zr0.1Ti0.9O3-0.15Bi(Zn2/3Ta1/3)O3 (BCZT-BZT) 薄膜。由于晶格不匹配,所有薄膜都由不同比例的应变层和松弛层组成,应变层被认为会降低薄膜的耐电压性。J-E 曲线结果表明,BCZT-BZT60 和 BCZT-BZT65 的传导机制从肖特基发射过渡到欧姆接触,并在底部形成了电阻率较高的耗尽层。考虑到从 TEM 图像中直接观察到的从 T 相到 O 相的自下而上的相演化,我们认为这两种薄膜中会出现电场随电压耐力而重新分布的现象,数学推导也证实了这一点。应变层和松弛层之间的变化以及传导机制的转变所产生的协同效应,使 BCZT-BZT65 的击穿强度(Eb)达到最高的 7.01 MV cm-1,可恢复能量密度(Wrec)达到 101.79 J cm-3。此外,BCZT-BZT65 在恶劣环境中表现出高度可靠性和卓越的放电性能,放电时间(t0.9)仅为 0.45 μs。
Revealing the effect of conductive mechanism on the voltage endurance of ferroelectric thin films via controlling the deposition temperature for reaching high energy storage capability†
Dielectric capacitors are considered superior to Li-ion batteries for replacing conventional internal combustion engines because they have no drawbacks of long charging times. Compared to the material's state of bulk ceramics and flexible composite films, dielectric capacitors in the form of thin films offer greater flexibility for regulation beyond domain and interface engineering. In this work, we grew 0.75Ba0.15Ca0.85Zr0.1Ti0.9O3–0.15Bi(Zn2/3Ta1/3)O3 (BCZT–BZT) thin films on 100 nm SrRuO3(SRO)-coated (001)-STO substrates at various deposition temperatures. Due to lattice mismatch, all films consist of a strained layer and a relaxed layer, with varying proportions, and the strained layer is considered to degrade the voltage endurance of the thin films. The J–E curve results indicate a conduction mechanism transition from Schottky emission to Ohmic contact, with the formation of a depletion layer, which is higher in resistivity, at the bottom of BCZT–BZT60 and BCZT–BZT65. Considering a phase evolution from T-phase to O-phase from the bottom up, directly observed in the TEM images, electric field redistribution with voltage endurance was thought to occur in these two thin films, which is confirmed by the mathematical derivation. The synergistic effects of the variation between the strained and relaxed layers, along with the transitions in the conduction mechanism, result in BCZT–BZT65 achieving the highest breakdown strength (Eb) of 7.01 MV cm−1 and a recoverable energy density (Wrec) of 101.79 J cm−3. Additionally, BCZT–BZT65 demonstrates high reliability in harsh environments and excellent discharge performance with a discharge time (t0.9) of only 0.45 μs.
期刊介绍:
The Journal of Materials Chemistry is divided into three distinct sections, A, B, and C, each catering to specific applications of the materials under study:
Journal of Materials Chemistry A focuses primarily on materials intended for applications in energy and sustainability.
Journal of Materials Chemistry B specializes in materials designed for applications in biology and medicine.
Journal of Materials Chemistry C is dedicated to materials suitable for applications in optical, magnetic, and electronic devices.
Example topic areas within the scope of Journal of Materials Chemistry C are listed below. This list is neither exhaustive nor exclusive.
Bioelectronics
Conductors
Detectors
Dielectrics
Displays
Ferroelectrics
Lasers
LEDs
Lighting
Liquid crystals
Memory
Metamaterials
Multiferroics
Photonics
Photovoltaics
Semiconductors
Sensors
Single molecule conductors
Spintronics
Superconductors
Thermoelectrics
Topological insulators
Transistors