Production of Al-based amorphous sheets with large thickness by a supercooled liquid-quenching method

1991 ◽  
Vol 10 (5) ◽  
pp. 289-291 ◽  
Author(s):  
M. Oguchi ◽  
A. Inoue ◽  
H. Yamaguchi ◽  
T. Masumoto
Materia Japan ◽  
1996 ◽  
Vol 35 (4) ◽  
pp. 415-417 ◽  
Author(s):  
Masahiro Oguchi ◽  
Yoshio Harakawa ◽  
Takayuki Matsuda ◽  
Akihisa Inoue ◽  
Tsuyoshi Masumoto

2020 ◽  
Vol 184 ◽  
pp. 109939
Author(s):  
Qingkang Liu ◽  
Longqiu Li ◽  
Yeau-Ren Jeng ◽  
Guangyu Zhang ◽  
Cijun Shuai ◽  
...  

2012 ◽  
Vol 48 (3) ◽  
pp. 277 ◽  
Author(s):  
Shengsheng ZHAO ◽  
Yu CHENG ◽  
Zhengkai CHANG ◽  
Tiegang WANG ◽  
Chao SUN

Materials ◽  
2021 ◽  
Vol 14 (4) ◽  
pp. 929
Author(s):  
Dandan Liang ◽  
Jo-Chi Tseng ◽  
Xiaodi Liu ◽  
Yuanfei Cai ◽  
Gang Xu ◽  
...  

This study investigated the structural heterogeneity, mechanical property, electrochemical behavior, and passive film characteristics of Fe–Cr–Mo–W–C–B–Y metallic glasses (MGs), which were modified through annealing at different temperatures. Results showed that annealing MGs below the glass transition temperature enhanced corrosion resistance in HCl solution owing to a highly protective passive film formed, originating from the decreased free volume and the shrinkage of the first coordination shell, which was found by pair distribution function analysis. In contrast, the enlarged first coordination shell and nanoscale crystal-like clusters were identified for MGs annealed in the supercooled liquid region, which led to a destabilized passive film and thereby deteriorated corrosion resistance. This finding reveals the crucial role of structural heterogeneity in tuning the corrosion performance of MGs.


2000 ◽  
Vol 655 ◽  
Author(s):  
Cesar Guerrero ◽  
Florencio Sánchez ◽  
José Roldán ◽  
Frank Güell ◽  
María V. García-Cuenca

AbstractA comparison of pulsed laser deposited PbZr0.53Ti0.47O3 (PZT) thin film capacitors with SrRuO3 (SRO) and LaNiO3 (LNO) electrodes on (001) yttria-stabilized zirconia (YSZ) and lattice matched (001) LaAlO3 substrates is presented. Both electrode materials allow for the formation of ferroelectric capacitors with large remnant polarization (20-30 μC/cm2) and negligible fatigue, although slight differences arise regarding the promotion of either the rhombohedral or tetragonal phases of PZT. Far more crucial seems to be the tendency of SrRuO3 to develop a rougher surface at either small (<30 nm) or large thickness (>100 nm), and on YSZ substrates. In those cases a highly defective and possibly low dielectric interface forms between the electrode and the ferroelectric layer, resulting in greatly degraded ferroelectric performance. LaNiO3 is free from these limitations except for the cracks forming at very large thickness (>300 nm), and therefore appears as a more versatile electrode material.


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