Effects of CeO2 buffer layer thickness on the orientation and dielectric properties of Ba(Zr0.20Ti0.80)O3 thin films

2009 ◽  
Vol 311 (2) ◽  
pp. 299-303 ◽  
Author(s):  
Lina Gao ◽  
Jiwei Zhai ◽  
Sangnian Song ◽  
Xihong Hao ◽  
Xi Yao
1994 ◽  
Vol 339 ◽  
Author(s):  
T. J. Kistenmacher ◽  
S. A. Ecelberger ◽  
W. A. Bryden

ABSTRACTIntroduction of a buffer layer to facilitate heteroepitaxy in thin films of the Group IIIA nitrides has had a tremendous impact on growth morphology and electrical transport. While AIN- and self-seeded growth of GaN has captured the majority of attention, the use of AIN-buffered substrates for InN thin films has also had considerable success. Herein, the properties of InN thin films grown by reactive magnetron sputtering on AIN-buffered (00.1) sapphire and (111) silicon are presented and, in particular, the evolution of the structural and electrical transport properties as a function of buffer layer sputter time (corresponding to thicknesses from ∼50Å to ∼0.64 μm) described. Pertinent results include: (a) for the InN overlayer, structural coherence and homogeneous strain normal to the (00.1) growth plane are highly dependent on the thickness of the AIN-buffer layer; (b) the homogeneous strain in the AIN-buffer layer is virtually nonexistent from a thickness of 200Å (where a significant X-ray intensity for (00.2)AIN is observed); and (c) the n-type electrical mobility for films on AIN-nucleated (00.1) sapphire is independent of AIN-buffer layer thickness, owing to divergent variations in carrier concentration and film resistivity. These effects are in the main interpreted as arising from a competition between the lattice mismatch of the InN overlayer with the substrate and with the AIN-buffer layer.


2004 ◽  
Vol 262 (1-4) ◽  
pp. 456-460 ◽  
Author(s):  
Yuantao Zhang ◽  
Guotong Du ◽  
Boyang Liu ◽  
HuiChao Zhu ◽  
Tianpeng Yang ◽  
...  

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