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Cited 10 time in webofscience Cited 12 time in scopus
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Memristive Devices from CuO Nanoparticlesopen access

Authors
Walke, Pundalik D.Rana, Abu ul Hassan SarwarYuldashev, Shavkat U.Magotra, Verjesh KumarLee, Dong JinAbdullaev, ShovkatKang, Tae WonJeon, Hee Chang
Issue Date
Sep-2020
Publisher
MDPI
Keywords
CuO nanomaterials; negative differential resistance; Poole-Frenkel conduction; switching ratio; resistive switching; space charge limited current
Citation
NANOMATERIALS, v.10, no.9, pp 1 - 10
Pages
10
Indexed
SCIE
SCOPUS
Journal Title
NANOMATERIALS
Volume
10
Number
9
Start Page
1
End Page
10
URI
https://scholarworks.dongguk.edu/handle/sw.dongguk/6198
DOI
10.3390/nano10091677
ISSN
2079-4991
2079-4991
Abstract
Memristive systems can provide a novel strategy to conquer the von Neumann bottleneck by evaluating information where data are located in situ. To meet the rising of artificial neural network (ANN) demand, the implementation of memristor arrays capable of performing matrix multiplication requires highly reproducible devices with low variability and high reliability. Hence, we present an Ag/CuO/SiO2/p-Si heterostructure device that exhibits both resistive switching (RS) and negative differential resistance (NDR). The memristor device was fabricated on p-Si and Indium Tin Oxide (ITO) substrates via cost-effective ultra-spray pyrolysis (USP) method. The quality of CuO nanoparticles was recognized by studying Raman spectroscopy. The topology information was obtained by scanning electron microscopy. The resistive switching and negative differential resistance were measured from current-voltage characteristics. The results were then compared with the Ag/CuO/ITO device to understand the role of native oxide. The interface barrier and traps associated with the defects in the native silicon oxide limited the current in the negative cycle. The barrier confined the filament rupture and reduced the reset variability. Reset was primarily influenced by the filament rupture and detrapping in the native oxide that facilitated smooth reset and NDR in the device. The resistive switching originated from traps in the localized states of amorphous CuO. The set process was mainly dominated by the trap-controlled space-charge-limited; this led to a transition into a Poole-Frenkel conduction. This research opens up new possibilities to improve the switching parameters and promote the application of RS along with NDR.
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