DocumentCode :
3102462
Title :
Uniformity improvement by optimization of switching interface in bi-layer unipolar RRAM structure for low power new memory application
Author :
Ryoo, Kyung-Chang ; Oh, Jeong-Hoon ; Jung, Sunghun ; Kim, Sungjun ; Park, Byung-Gook
Author_Institution :
Inter-Univ. Semicond. Res. Center (ISRC), Seoul Nat. Univ., Seoul, South Korea
fYear :
2011
fDate :
7-9 Dec. 2011
Firstpage :
1
Lastpage :
2
Abstract :
RRAM is very promising due to many fascinating advantages as follows; fast writing/reading time, low programming power and multi bit storage for high density up to tera bit memory are possible [1]. But it is very difficult to satisfy all best resistive switching characteristics. There is a trade-off between reset current (IRESET) and forming voltage (VFORMING) in single layered cell structure as shown in fig. 1 (a). Fig. 1 (b) shows the initial resistance (RINITIAL) as a function of reset resistance (RRESET) and set resistance (RSET) by using our fabricated NiO based unipolar RRAM cell. We have reported that VFORMING increases if RINITIAL is high enough, therefore it proves that RINITIAL needs to be lowered in order to lower operating condition [2]. However there is also a trade off. If RINITIAL is sufficiently low, sensing margin which means reset/set resistance ratio is also reduced. So, new ideas for satisfying both resistive switching conditions are needed. Figure 2 shows the typical I-V curves of forming (a) and reset/set switching (b) based on single layered unipolar RRAM structure by using RCB model [3] and figure 3 shows the illustration of bi layered RRAM cell structure. Lower layer (2ND resistive layer) is acting as forming assistance layer for low power consumption. Upper layer (1ST resistive layer) is used for controlling reset/set switching. Because resistive switching occurs at cell interface, interface engineering is very critical for improving resistive switching uniformity. Figure 4 illustrates the detailed tested metal - insulator-metal (MIM) cell structure. Charged particle which is source of CF path such as oxygen vacancy and metallic ion in resistive cell can be defined as conductive defect. Conductive defect fraction is varied from 0.05 (lower layer) to 0.025 (upper layer), respectively. Conductive defect fraction of referen- e cell is 0.05. The each layer rules and their actions for bi-layered RRAM cell structure are summarized in table 2. Figure 5 shows the statistical analysis of VFORMING (a) and VSET (b) characteristics with various cell conditions. Lower VFORMING is addressed in single layered cell due to its larger amount of conductive defects, but in case of 5nm thickness of upper layer (split 1) cell, mean value of forming voltage (VFORMING_μ) difference is only 0.26V.
Keywords :
MIM structures; random-access storage; CF path; MIM cell structure; RCB model; bilayer unipolar RRAM structure; low power new memory application; metal-insulator-metal cell structure; optimal upper layer thickness; optimization; reset-set resistance ratio; resistive switching characteristics; single layered cell structure; switching interface; uniformity improvement; voltage 0.26 V; Educational institutions; Periodic structures; Resistance; Statistical analysis; Switches; Switching circuits;
fLanguage :
English
Publisher :
ieee
Conference_Titel :
Semiconductor Device Research Symposium (ISDRS), 2011 International
Conference_Location :
College Park, MD
Print_ISBN :
978-1-4577-1755-0
Type :
conf
DOI :
10.1109/ISDRS.2011.6135405
Filename :
6135405
Link To Document :
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