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中国物理学会期刊

VO2纳米粒子填充型聚合物薄膜电致相变特性

CSTR: 32037.14.aps.69.20200834

Voltage induced phase transition of polyethene glycol composite film filled with VO2 nanoparticles

CSTR: 32037.14.aps.69.20200834
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  • 采用简单的水热法结合热处理工艺, 制备了高纯、形貌可控的纳米VO2 (M)颗粒, 得到了退火时间对颗粒形貌的影响, 首次揭示了VO2聚乙二醇复合薄膜电致相变过程, 建立了电致相变模型. 实验以V2O5和H2C2O4·2H2O为原料, 经180 ℃, 12 h水热处理后, 得到VO2 (B)纳米颗粒, 真空退火转化为VO2 (M). 结果表明, 退火时间越长, 纳米颗粒长度越短. 多次重复测试发现, 复合薄膜在电场作用下, 均能够发生显著的相变现象, 但同一样品的重复相变电压低于第1次测试数据. 在首次测试后, 相变电压和非线性系数随纳米VO2的长度减小而指数增加, 同时发现材料两端电压在相变后可维持在10 V附近. 分析认为, 复合薄膜的相变电压和非线性系数由颗粒内势垒和界面间势垒共同决定. 首次伏安测试降低了颗粒间势垒, 造成了材料的“激活”现象, 纳米颗粒平均长度越短, 导电通道中的界面间势垒越多, 导致相变电压和非线性系数升高. 实验发现, 电场作用是复合薄膜相变发生的决定因素, 相变后焦耳热对维持相变起主要作用.

     

    In this paper, the voltage induced metal-insulator phase transition (MIT) of polyethene glycol (PEG) composite film is investigated based on VO2 nanoparticles prepared by the hydrothermal method and vacuum annealing process. High purity VO2 (B) nanoparticles are obtained after being treated in a hydrothermal reactor at 180 ℃ for 12 h by using vanadium pentoxide (V2O5) and oxalic acid (H2C2O4·2H2O) as raw materials. The X-ray diffraction (XRD) pattern shows that the prepared nano-powders are free of impurities, and the scanning electron microscope (SEM) pictures confirm that the micro-morphology is of a band-shaped nano-structure. Next, these products are heated in a vacuum quartz tube at 500 ℃ for different times. The XRD and differential scanning calorimeter (DSC) curves of the annealed samples prove that the VO2 (M) with MIT performance is successfully prepared. And the content of M phase in the sample increases with preparation time increasing. When the annealing time is longer than 60 min, all the samples are converted into materials with M phase. The SEM images show that the average length of the nano-powders decreases with the annealing time increasing from 10 min to 300 min. Then PEG coating containing VO2 (M) nanoparticles is applied between two electrodes with a pitch of 1 mm on printed circuit board (PCB). The V-I test is carried out after a 20 kΩ resistor has been connected in the circuit. The results display repeatable non-linear V-I curves indicating that the composite film undergoes an MIT phase transition under voltage. After it is activated for the first test, the MIT voltage and non-linear coefficient increase exponentially as the length of VO2 decreases. Besides, it is also found that the voltage across the material is maintained at around 10 V after the resistance has changed suddenly, which is similar to the behavior of diode clamping voltage. We believe that the phase transition voltage and non-linear coefficient of the VO2 composite film are influenced by the intra-particle potential barrier and the inter-layer potential barrier. The longer the average length of the nanoparticles, the higher the potential barrier between the interfaces in the conductive channels is, and thus increasing the phase transition voltage and phase transition coefficient. The activation phenomenon of the thin film is caused by reducing the barrier between particles during the first test. Furthermore, the results can prove that the electric field is the determinant of the phase transition during the VO2 composite film electrical field induced MIT of the VO2 composite film. However, after the phase transition, Joule heat plays a significant role in maintaining the low resistance state.

     

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