Dual Functions of V/SiO x /AlO y /p++Si Device as Selector and Memory

Abstract This letter presents dual functions including selector and memory switching in a V/SiO x /AlO y /p++Si resistive memory device by simply controlling compliance current limit (CCL). Unidirectional threshold switching is observed after a positive forming with low CCL of 1 μA. The shifts to th...

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Main Authors: Sungjun Kim, Chih-Yang Lin, Min-Hwi Kim, Tae-Hyeon Kim, Hyungjin Kim, Ying-Chen Chen, Yao-Feng Chang, Byung-Gook Park
Format: Article
Language:English
Published: SpringerOpen 2018-08-01
Series:Nanoscale Research Letters
Subjects:
Online Access:http://link.springer.com/article/10.1186/s11671-018-2660-9
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author Sungjun Kim
Chih-Yang Lin
Min-Hwi Kim
Tae-Hyeon Kim
Hyungjin Kim
Ying-Chen Chen
Yao-Feng Chang
Byung-Gook Park
author_facet Sungjun Kim
Chih-Yang Lin
Min-Hwi Kim
Tae-Hyeon Kim
Hyungjin Kim
Ying-Chen Chen
Yao-Feng Chang
Byung-Gook Park
author_sort Sungjun Kim
collection DOAJ
description Abstract This letter presents dual functions including selector and memory switching in a V/SiO x /AlO y /p++Si resistive memory device by simply controlling compliance current limit (CCL). Unidirectional threshold switching is observed after a positive forming with low CCL of 1 μA. The shifts to the V-electrode side of the oxygen form the VO x layer, where the threshold switching can be explained by the metal-insulation-transition phenomenon. For higher CCL (30 μA) applied to the device, a bipolar memory switching is obtained, which is attributed to formation and rupture of the conducting filament in SiO y layer. 1.5-nm-thick AlO y layer with high thermal conductivity plays an important role in lowering the off-current for memory and threshold switching. Through the temperature dependence, high-energy barrier (0.463 eV) in the LRS is confirmed, which can cause nonlinearity in a low-resistance state. The smaller the CCL, the higher the nonlinearity, which provides a larger array size in the cross-point array. The coexistence of memory and threshold switching in accordance with the CCL provides the flexibility to control the device for its intended use.
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spelling doaj.art-29b765da25f24417a6a2a4c8125a7f082023-09-02T23:36:15ZengSpringerOpenNanoscale Research Letters1931-75731556-276X2018-08-011311710.1186/s11671-018-2660-9Dual Functions of V/SiO x /AlO y /p++Si Device as Selector and MemorySungjun Kim0Chih-Yang Lin1Min-Hwi Kim2Tae-Hyeon Kim3Hyungjin Kim4Ying-Chen Chen5Yao-Feng Chang6Byung-Gook Park7School of Electronics Engineering, Chungbuk National UniversityDepartment of Physics, National Sun Yat-sen UniversityDepartment of Electrical and Computer Engineering, Inter-University Semiconductor Research Center (ISRC), Seoul National UniversityDepartment of Electrical and Computer Engineering, Inter-University Semiconductor Research Center (ISRC), Seoul National UniversityDepartment of Electrical and Computer Engineering, Inter-University Semiconductor Research Center (ISRC), Seoul National UniversityDepartment of Electrical and Computer Engineering, Microelectronics Research Center, University of Texas at AustinIntel CorporationDepartment of Electrical and Computer Engineering, Inter-University Semiconductor Research Center (ISRC), Seoul National UniversityAbstract This letter presents dual functions including selector and memory switching in a V/SiO x /AlO y /p++Si resistive memory device by simply controlling compliance current limit (CCL). Unidirectional threshold switching is observed after a positive forming with low CCL of 1 μA. The shifts to the V-electrode side of the oxygen form the VO x layer, where the threshold switching can be explained by the metal-insulation-transition phenomenon. For higher CCL (30 μA) applied to the device, a bipolar memory switching is obtained, which is attributed to formation and rupture of the conducting filament in SiO y layer. 1.5-nm-thick AlO y layer with high thermal conductivity plays an important role in lowering the off-current for memory and threshold switching. Through the temperature dependence, high-energy barrier (0.463 eV) in the LRS is confirmed, which can cause nonlinearity in a low-resistance state. The smaller the CCL, the higher the nonlinearity, which provides a larger array size in the cross-point array. The coexistence of memory and threshold switching in accordance with the CCL provides the flexibility to control the device for its intended use.http://link.springer.com/article/10.1186/s11671-018-2660-9Resistive switchingSelectorMemoryNonlinearitySilicon oxideVanadium
spellingShingle Sungjun Kim
Chih-Yang Lin
Min-Hwi Kim
Tae-Hyeon Kim
Hyungjin Kim
Ying-Chen Chen
Yao-Feng Chang
Byung-Gook Park
Dual Functions of V/SiO x /AlO y /p++Si Device as Selector and Memory
Nanoscale Research Letters
Resistive switching
Selector
Memory
Nonlinearity
Silicon oxide
Vanadium
title Dual Functions of V/SiO x /AlO y /p++Si Device as Selector and Memory
title_full Dual Functions of V/SiO x /AlO y /p++Si Device as Selector and Memory
title_fullStr Dual Functions of V/SiO x /AlO y /p++Si Device as Selector and Memory
title_full_unstemmed Dual Functions of V/SiO x /AlO y /p++Si Device as Selector and Memory
title_short Dual Functions of V/SiO x /AlO y /p++Si Device as Selector and Memory
title_sort dual functions of v sio x alo y p si device as selector and memory
topic Resistive switching
Selector
Memory
Nonlinearity
Silicon oxide
Vanadium
url http://link.springer.com/article/10.1186/s11671-018-2660-9
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