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ε‐Ga(2)O(3): An Emerging Wide Bandgap Piezoelectric Semiconductor for Application in Radio Frequency Resonators

The explosion of mobile data from the internet of things (IoT) is leading to the emergence of 5G technology with dramatic frequency band expansion and efficient band allocations. Along with this, the demand for high‐performance filters for 5G radio frequency (RF) front‐ends keeps growing. The most p...

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Detalles Bibliográficos
Autores principales: Chen, Zimin, Lu, Xing, Tu, Yujia, Chen, Weiqu, Zhang, Zhipeng, Cheng, Shengliang, Chen, Shujian, Luo, Hongtai, He, Zhiyuan, Pei, Yanli, Wang, Gang
Formato: Online Artículo Texto
Lenguaje:English
Publicado: John Wiley and Sons Inc. 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9661831/
https://www.ncbi.nlm.nih.gov/pubmed/36156466
http://dx.doi.org/10.1002/advs.202203927
Descripción
Sumario:The explosion of mobile data from the internet of things (IoT) is leading to the emergence of 5G technology with dramatic frequency band expansion and efficient band allocations. Along with this, the demand for high‐performance filters for 5G radio frequency (RF) front‐ends keeps growing. The most popular 5G filters are constructed by piezoelectric resonators based on AlN semiconductor. However, AlN possesses a piezoelectric constant d (33) lower than 5 pm V(−1) and it becomes necessary to develop novel semiconductors with larger piezoelectric constant. In this work, it is shown that strong piezoelectricity exists in ε‐Ga(2)O(3). High‐quality phase‐pure ε‐Ga(2)O(3) thin films with a relatively low residual stress are prepared. A switching spectroscopy piezoelectric force microscope (SS‐PFM) measurement is carried out and the piezoelectric constant d (33) of ε‐Ga(2)O(3) is determined to be ≈10.8–11.2 pm V(−1), which is twice as large as that of AlN. For the first time, surface acoustic wave (SAW) resonators are demonstrated on the ε‐Ga(2)O(3) thin films and different vibration modes resonating in the GHz range are observed. The results suggest that ε‐Ga(2)O(3) is a great material candidate for application in piezoelectric devices, thanks to its wide bandgap, strong piezoelectric property, small acoustic impedance, and low residual stress.