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Cited 1 time in webofscience Cited 1 time in scopus
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Multifunctional HfAlO thin film: Ferroelectric tunnel junction and resistive random access memory

Authors
Park, YongjinLee, Jong-HoLee, Jung-KyuKim, Sungjun
Issue Date
Feb-2024
Publisher
AIP Publishing
Keywords
Dielectric Films; Ferroelectric Films; Ferroelectricity; Hafnium Compounds; Rram; Thin Films; Tunnel Junctions; 1/f Noise; 1/f-noise; Conductive Filaments; Ferroelectric Tunnel Junctions; High-resistance State; Low-resistance State; Noise Components; Noise Power; Random Access Memory; Resistance State; Aluminum Compounds; Article; Depression; Electric Potential; Human; Memory; Noise; Pattern Recognition; Pink Noise; Simulation
Citation
The Journal of Chemical Physics, v.160, no.7, pp 1 - 9
Pages
9
Indexed
SCIE
SCOPUS
Journal Title
The Journal of Chemical Physics
Volume
160
Number
7
Start Page
1
End Page
9
URI
https://scholarworks.dongguk.edu/handle/sw.dongguk/20636
DOI
10.1063/5.0190195
ISSN
0021-9606
1089-7690
Abstract
This study presents findings indicating that the ferroelectric tunnel junction (FTJ) or resistive random-access memory (RRAM) in one cell can be intentionally selected depending on the application. The HfAlO film annealed at 700 degrees C shows stable FTJ characteristics and can be converted into RRAM by forming a conductive filament inside the same cell, that is, the process of intentionally forming a conductive filament is the result of defect generation and redistribution, and applying compliance current prior to a hard breakdown event of the dielectric film enables subsequent RRAM operation. The converted RRAM demonstrated good memory performance. Through current-voltage fitting, it was confirmed that the two resistance states of the FTJ and RRAM had different transport mechanisms. In the RRAM, the 1/f noise power of the high-resistance state (HRS) was about ten times higher than that of the low-resistance state (LRS). This is because the noise components increase due to the additional current paths in the HRS. The 1/f noise power according to resistance states in the FTJ was exactly the opposite result from the case of the RRAM. This is because the noise component due to the Poole-Frenkel emission is added to the noise component due to the tunneling current in the LRS. In addition, we confirmed the potentiation and depression characteristics of the two devices and further evaluated the accuracy of pattern recognition through a simulation by considering a dataset from the Modified National Institute of Standards and Technology.
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