scholarly journals Growth mechanism and diffusion barrier property of plasma-enhanced atomic layer deposition Ti–Si–N thin films

Author(s):  
Jin-Seong Park ◽  
Sang-Won Kang ◽  
H. Kim
RSC Advances ◽  
2015 ◽  
Vol 5 (29) ◽  
pp. 22712-22717 ◽  
Author(s):  
Soumyadeep Sinha ◽  
Devika Choudhury ◽  
Gopalan Rajaraman ◽  
Shaibal K. Sarkar

DFT study of the growth mechanism of atomic layer deposited Zn3N2 thin film applied as a channel layer of TFT.


2012 ◽  
Vol 329 ◽  
pp. 159-164 ◽  
Author(s):  
Rosniza Hussin ◽  
Xiang Hui Hou ◽  
Kwang Leong Choy

Atomic Layer Deposition (ALD) Offers the Key Benefits of Precise Deposition of Nanostructured Thin Films with Excellent Conformal Coverage. ALD Is Being Used in the Semiconductor Industry for Producing High-k (high Permittivity) Gate Oxides and High-K Memory Capacitor Dielectrics. Zno Has Attractive Properties for Various Applications such as Semiconductors, Gas Sensors and Solar Cells. in this Study, ZnO Thin Films Were Deposited via ALD Using Alternating Exposures of Diethyl Zinc (DEZ) and Deionized Water (H2O) on Silicon Wafer (100). the Thin Films Were Analyzed Using X-Ray Diffraction (XRD), Ellipsometer and Atomic Force Microscope (AFM). the XRD Analysis Shows the Presence of ZnO Thin Films with a Hexagonal Wurtzite Structure. the Thickness of ZnO Thin Films Was Correlated with the Substrate Temperatures and Deposition Cycles. the Coating Thickness Was Found to Increase with the Increase of the Deposition Cycles, but it Decreased with the Increase of Deposition Temperature. the Nucleation and Growth Mechanism of Zno Thin Film Has Been Established. it Can Be Concluded that, the Growth Mechanism of Zno Films Is Strongly Dependent on the ALD Processing Conditions.


2011 ◽  
Vol 519 (10) ◽  
pp. 3146-3154 ◽  
Author(s):  
Tommi O. Kääriäinen ◽  
Philipp Maydannik ◽  
David C. Cameron ◽  
Kimmo Lahtinen ◽  
Petri Johansson ◽  
...  

2002 ◽  
Vol 716 ◽  
Author(s):  
H. Kim ◽  
C. Cabral ◽  
C. Lavoie ◽  
S.M. Rossnagel

AbstractTa films were grown by plasma-enhanced atomic layer deposition (PE-ALD) at temperatures from room temperature up to 300 °C using TaCl5 as source gas and RF plasma-produced atomic H as the reducing agent. Post-deposition ex situ chemical analyses showed that the main impurity is oxygen, incorporated during the air exposure prior to analysis with typically low Cl concentration below 1 at %. The X-ray diffraction indicates that ALD Ta films are amorphous or composed of nano-grains. The typical resistivity of ALD Ta films was 150-180 μΩ cm, which corresponds to that of β-Ta phase, at a wide range of growth parameters. The conformality of the film is 100 % up to an aspect ratio of 15:1 and 40 % for aspect ratio of 40:1. The thickness per cycle, corresponding to the growth rate, was measured by Rutherford back scattering as a function of various key growth parameters, including TaCl5 and H exposure time and growth temperature. The maximum thickness per cycle values were below 0.1 ML, probably due to the steric hindrance for TaCl5 adsorption. Bilayer structures consisting of Cu films deposited by sputtering and ALD Ta films with various thicknesses were prepared and the diffusion barrier properties of ALD Ta films were investigated by various analysis techniques consisting of X-ray diffraction, elastic light scattering, and resistance analysis. The results were compared with Ta thin films deposited by sputtering with comparable thicknesses. Also, the growth of TaN films by PE-ALD using consecutive exposures of atomic H and activated N2 is presented.


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