Design of High-k Interfacial Layer Formation by Cycle-by-Cycle Deposition and Annealing Method

2019 ◽  
Vol 19 (2) ◽  
pp. 129-143 ◽  
Author(s):  
Arito Ogawa ◽  
Kunihiko Iwamoto ◽  
Hiroyuki Ota ◽  
Masashi Takahashi ◽  
Akito Hirano ◽  
...  
2020 ◽  
Vol 223 ◽  
pp. 111219 ◽  
Author(s):  
S. Siddiqui ◽  
R. Galatage ◽  
W. Zhao ◽  
G. Raja Muthinti ◽  
J. Fronheiser ◽  
...  

2001 ◽  
Vol 666 ◽  
Author(s):  
V. Craciun ◽  
N. D. Bassim ◽  
J. M. Howard ◽  
J. Spear ◽  
S. Bates ◽  
...  

ABSTRACTYttrium oxide and barium strontium titanate (BST) thin films were grown directly on Si substrates by the pulsed laser deposition (PLD) technique. Because the optimum oxygen pressure during PLD process is of the order of 10 mTorr, some of the oxygen atoms are trapped inside the grown films and contribute to the growth of a silicon oxide interfacial layer. The use of an UV source during the growth resulted in the reduction of the optimum oxygen pressure and, as a consequence, the amount of trapped oxygen and thickness of the interfacial layer. In addition to that, UV radiation influenced the film morphologies and electrical properties. A further reduction of the interfacial layer was obtained on substrates that were exposed prior to deposition to NH3 for short periods of time under UV radiation.


2003 ◽  
Vol 765 ◽  
Author(s):  
S. Van Elshocht ◽  
R. Carter ◽  
M. Caymax ◽  
M. Claes ◽  
T. Conard ◽  
...  

AbstractBecause of aggressive downscaling to increase transistor performance, the physical thickness of the SiO2 gate dielectric is rapidly approaching the limit where it will only consist of a few atomic layers. As a consequence, this will result in very high leakage currents due to direct tunneling. To allow further scaling, materials with a k-value higher than SiO2 (“high-k materials”) are explored, such that the thickness of the dielectric can be increased without degrading performance.Based on our experimental results, we discuss the potential of MOCVD-deposited HfO2 to scale to (sub)-1-nm EOTs (Equivalent Oxide Thickness). A primary concern is the interfacial layer that is formed between the Si and the HfO2, during the MOCVD deposition process, for both H-passivated and SiO2-like starting surfaces. This interfacial layer will, because of its lower k-value, significantly contribute to the EOT and reduce the benefit of the high-k material. In addition, we have experienced serious issues integrating HfO2 with a polySi gate electrode at the top interface depending on the process conditions of polySi deposition and activation anneal used. Furthermore, we have determined, based on a thickness series, the k-value for HfO2 deposited at various temperatures and found that the k-value of the HfO2 depends upon the gate electrode deposited on top (polySi or TiN).Based on our observations, the combination of MOCVD HfO2 with a polySi gate electrode will not be able to scale below the 1-nm EOT marker. The use of a metal gate however, does show promise to scale down to very low EOT values.


2007 ◽  
Vol 42 (17) ◽  
pp. 7343-7347 ◽  
Author(s):  
Ran Jiang ◽  
E. Q. Xie ◽  
Z. F. Wang

2012 ◽  
Vol 51 ◽  
pp. 081303 ◽  
Author(s):  
Shinya Hibino ◽  
Tomonori Nishimura ◽  
Kosuke Nagashio ◽  
Koji Kita ◽  
Akira Toriumi

2015 ◽  
Vol 138 ◽  
pp. 81-85 ◽  
Author(s):  
Dun-Bao Ruan ◽  
Kuei-Shu Chang-Liao ◽  
Chen-Chien Li ◽  
Chun-Chang Lu ◽  
Yu-Liang Liao ◽  
...  

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