ferroelectric film
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2022 ◽  
Author(s):  
Eugene A. Eliseev ◽  
Mykola E. Yelisieiev ◽  
Sergei V. Kalinin ◽  
Anna N. Morozovska

2022 ◽  
Vol 2160 (1) ◽  
pp. 012018
Author(s):  
Minglong Zhai ◽  
Xueyuan Liu ◽  
Hudong Chang ◽  
Honggang Liu ◽  
Bing Sun

Abstract The capping layers have great influences on the ferroelectricity of the Hf0.5Zr05O2 (HZO) film during annealing process. In this paper we compared the properties of the HZO film with two inorganic nonmetallic capping layers and no capping layer. The remnant (2Pr) of HZO films are 23.5 uC/cm2, 27.3 uC/cm2 and 20.3 uC/cm2 for no capping layer, Si3N4 capping layer and SiO2 capping layer, respectively. The capping layer can change the direction of the coercive filed shift even though the capacitors have the same metal electrodes.


2021 ◽  
Vol 21 (9) ◽  
pp. 4911-4915
Author(s):  
Sheik Abdur Rahman ◽  
Muhammad Saqib ◽  
Shenawar Ali Khan ◽  
Hafiz Mohammad Mutee Ur Rehman ◽  
Woo Young Kim

A metal/insulator/ferroelectric/metal structure was fabricated using a covering of approximately 10 nm thick of an insulating polystyrene film on a ferroelectric poly(vinylidene fluoride-trifluoroethylene) film. To fabricate several samples, the thickness of the ferroelectric film was held constant while the thickness of the insulating film was varied from 8 to 24 nm. The polarization– voltage relationships were measured to extract the main parameters, in this case the remanent polarization, depolarization, coercive voltage and biased voltage values. As the insulating film becomes thicker, the remanent polarization and coercive voltage values tended to increase. On the other hand, depolarization and biased voltage values decreased. By analyzing the above mentioned parameters, a certain optimum insulator thickness could be predicted. This work shows that metal/insulator/ferroelectric/metal devices are more useful than metal/ferroelectric/metal capacitors.


2021 ◽  
Author(s):  
Mohamed M. Mansour ◽  
Haruichi Kanaya

Tunable microwave devices have the benefits of added functionality, smaller form factor, lower cost, and lightweight, and are in great demand for future communications and radar applications as they can extend the operation over a wide dynamic range. Current tunable technologies include several schemes such as ferrites, semiconductors, microelectromechanical systems (MEMS), and ferroelectric thin films. While each technology has its own pros and cons, ferroelectric thin film-based technology has proved itself as the potential candidate for tunable devices due to its simple processes, low power consumption, high power handling, small size, and fast tuning. A tunable Composite Right Left-Handed Zeroth Order Resonator (CRLH ZOR) is introduced in this chapter and it relies mainly on the latest advancement in the ferroelectric materials. It is common that for achieving optimum performance for the resonant structure, this involves the incorporation of an additional tuning by either mechanical means (i.e. with tuning screws) or other coupling mechanisms. The integration between electronic tuning and High-Temperature Superconducting (HTS) components yields a high system performance without degradation of efficiency. This leads not only low-loss microwave components that could be fine-tuned for maximum efficiency but will provide a tunable device over a broadband frequency spectrum as well. The dielectric properties of the ferroelectric thin film, and the thickness of the ferroelectric film, play a fundamental role in the frequency or phase tunability and the overall insertion loss of the circuit. The key advantages of using ferroelectric are the potential for significant size-reduction of the microwave components and systems and the cabibility for integration with microelectronic circuits due to the utilization of thin and thick ferroelectric film technology. In this chapter, ZOR is discussed and the conceptual operation is introduced. The ZOR is designed and simulated by the full-wave analysis software. The response is studied using electromagnetic characteristics with the applied electric field, ferroelectric thickness, and the operating temperature.


AIP Advances ◽  
2021 ◽  
Vol 11 (6) ◽  
pp. 065202
Author(s):  
Pan Zhang ◽  
Wenjing Zhai ◽  
Zhibo Yan ◽  
Xiang Li ◽  
Yongqiang Li ◽  
...  

2021 ◽  
Vol 571 (1) ◽  
pp. 200-206
Author(s):  
X.-D. Meng ◽  
L.-Z. Chu ◽  
Z.-C. Deng ◽  
P.-C. Zhang ◽  
Y.-L. Wang

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