Effect of Thermal Annealing on Nonvolatile Memory Structures Containing a High-k La2O3 Charge-trapping Layer

2011 ◽  
Vol 58 (2) ◽  
pp. 264-269 ◽  
Author(s):  
Dong Hak Kim ◽  
Joon Won Park ◽  
Chang-Oh Kim ◽  
Haeyang Chung ◽  
Suk-Ho Choi ◽  
...  
2010 ◽  
Vol 1250 ◽  
Author(s):  
Nikolaos Nikolaou ◽  
Panos Dimitrakis ◽  
Pascal Normand ◽  
Konstantinos Giannakopoulos ◽  
Konstantina Mergia ◽  
...  

AbstractIn this work, we examine the influence of hafnium and zirconium oxides ALD precursor chemistry on the memory properties of SiO2/Si3N4/ZrO2 and SiO2/Si3N4/HfO2 non-volatile gate memory stacks. Approximately 10 nm thick ZrO2 and HfO2 layers were deposited on top of a SiO2/Si3N4 structure, functioning as blocking oxides. Both metal oxides were deposited using either alkylamides or cyclopentadienyls as metal precursors, and ozone as the oxygen source. In the case of the ZrO2 gate stacks a memory window of 6 V was determined, comprised of 4 V write window and 2 V erase window. Although no dramatic differences were evident between the ZrO2 layers, ZrO2 grown from alkylamide provided structures with higher dielectric strength. The memory structures with HfO2 blocking layers indicate that the memory window and the dielectric strength are significantly affected by the precursor. The structures with the HfO2 formed from alkylamide showed a write window of 7 V, while the films grown from cyclopentadienyl possessed window of 5 V. Comparison between the memory windows obtained using ZrO2 and HfO2 as control oxides reveals that the former provides memory structures with higher electron trapping efficiency.


2013 ◽  
Vol 1562 ◽  
Author(s):  
Chi-Chou Lin ◽  
Yue Kuo

ABSTRACTMOS capacitor composed of nc-CdSe embedded ZrHfO high-k gate dielectric stack was fabricated and characterized for nonvolatile memory functions. Detailed material and electrical properties have been investigated. With a large charge trapping capability, this kind of device can trap electrons or holes depending on the polarity and magnitude of the applied gate voltage. For the same stress time, the device trapped more holes than electrons under the same magnitude of gate voltage but different polarity. The negative differential resistance peak was observed at the room temperature due to the Coulomb blockade effect. The charge trapping mechanism was delineated with the constant voltage stress test. After 10 years of storage, about 56% of trapped charges still remain in the device.


2008 ◽  
Vol 92 (17) ◽  
pp. 173506 ◽  
Author(s):  
Tung-Ming Pan ◽  
Wen-Wei Yeh

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