TY - GEN
T1 - Uniformity improvement by optimization of switching interface in bi-layer unipolar RRAM structure for low power new memory application
AU - Ryoo, Kyung Chang
AU - Oh, Jeong Hoon
AU - Jung, Sunghun
AU - Kim, Sungjun
AU - Park, Byung Gook
PY - 2011
Y1 - 2011
N2 - 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 (I RESET) and forming voltage (V FORMING) in single layered cell structure as shown in fig. 1 (a). Fig. 1 (b) shows the initial resistance (R INITIAL) as a function of reset resistance (R RESET) and set resistance (R SET) by using our fabricated NiO based unipolar RRAM cell. We have reported that V FORMING increases if R INITIAL is high enough, therefore it proves that R INITIAL needs to be lowered in order to lower operating condition [2]. However there is also a trade off. If R INITIAL 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 (2 ND resistive layer) is acting as forming assistance layer for low power consumption. Upper layer (1 ST 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 reference 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 V FORMING (a) and V SET (b) characteristics with various cell conditions. Lower V FORMING 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 (V FORMING-) difference is only 0.26V.
AB - 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 (I RESET) and forming voltage (V FORMING) in single layered cell structure as shown in fig. 1 (a). Fig. 1 (b) shows the initial resistance (R INITIAL) as a function of reset resistance (R RESET) and set resistance (R SET) by using our fabricated NiO based unipolar RRAM cell. We have reported that V FORMING increases if R INITIAL is high enough, therefore it proves that R INITIAL needs to be lowered in order to lower operating condition [2]. However there is also a trade off. If R INITIAL 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 (2 ND resistive layer) is acting as forming assistance layer for low power consumption. Upper layer (1 ST 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 reference 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 V FORMING (a) and V SET (b) characteristics with various cell conditions. Lower V FORMING 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 (V FORMING-) difference is only 0.26V.
UR - http://www.scopus.com/inward/record.url?scp=84863141929&partnerID=8YFLogxK
U2 - 10.1109/ISDRS.2011.6135405
DO - 10.1109/ISDRS.2011.6135405
M3 - Conference contribution
AN - SCOPUS:84863141929
SN - 9781457717550
T3 - 2011 International Semiconductor Device Research Symposium, ISDRS 2011
BT - 2011 International Semiconductor Device Research Symposium, ISDRS 2011
T2 - 2011 International Semiconductor Device Research Symposium, ISDRS 2011
Y2 - 7 December 2011 through 9 December 2011
ER -