Substrate biasing effect on the electrical properties of magnetron-sputtered high-k titanium silicate thin films

2007 ◽  
Vol 102 (3) ◽  
pp. 034106 ◽  
Author(s):  
D. Brassard ◽  
M. A. El Khakani ◽  
L. Ouellet
2019 ◽  
Vol 28 (1) ◽  
pp. 125-135 ◽  
Author(s):  
Steven P. Consiglio ◽  
Cory Wajda ◽  
Genji Nakamura ◽  
Robert Clark ◽  
Shintaro Aoyama ◽  
...  

2011 ◽  
Vol 125 (1) ◽  
pp. 44-52 ◽  
Author(s):  
S. P. Pavunny ◽  
R. Thomas ◽  
N. M. Murari ◽  
J. Schubert ◽  
V. Niessen ◽  
...  

2012 ◽  
Vol 195 ◽  
pp. 95-97
Author(s):  
Matthias Müller ◽  
Sonja Sioncke ◽  
Annelies Delabie ◽  
Burkhard Beckhoff

Thin films of high-k material are becoming more and more used for semiconductor devices. A further shrinking of the devices requires also a further reduction of the high-k film thickness. With this reduction of the high-k thickness down to just a few nanometers two technical challenges have to be addressed. The first one is the ALD process for the deposition of the high-k material. Usually the ALD process can be well controlled by tuning the number of process cycles. But it is theoretically predicted [1] that the growth-per-cycle of the first cycles can be different than the steady growth-per-cycle which is obtained for high cycle numbers. This effect is caused by a not fully covered initial surface during the first cycles. Only when the deposited material forms a closed surface and the surface probabilities are the same for each following cycle the deposition rate will be constant. The second challenge is that the electrical properties of thin films with a thickness of a few nanometers are significantly determined by the quality of the interface between the film and the substrate.


2000 ◽  
Vol 611 ◽  
Author(s):  
James J. Chambers ◽  
Gregory N. Parsons

ABSTRACTThis article reports on the physical and electrical properties of yttrium silicate, which is a possible high-k replacement for the SiO2 gate dielectric in CMOS devices. The yttrium silicate (Y-O-Si) films are formed by sputtering yttrium onto clean silicon, annealing in vacuum to form yttrium silicide and then oxidizing in N2O to form the silicate. Shifts in the Y 3d, Si 2p and O 1s photoelectron spectra with respect to Y2O3 and SiO2 indicate that the films are fully oxidized yttrium silicate. FTIR results that reveal a Si-O stretching mode at 950 cm−1 and Y-O stretching modes in the far-IR are consistent with XPS. XPS and FTIR results are in accordance with the donation of electron density from the yttrium to the Si-O bond in the silicate. The yttrium silicate films contain a fixed charge density of ∼9×1010 cm−2 negative charges as calculated from measured C-V behavior. The properties of ultra-thin yttrium silicate films with an equivalent silicon dioxide thickness (electrical) of ∼1.0 nm will be discussed elsewhere.


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