scholarly journals Resistivity of Cu, Ni and Sb in undercooled liquid state

2021 ◽  
Vol 1885 (3) ◽  
pp. 032010
Author(s):  
Fengxiang Guo ◽  
Xueyu Zhang ◽  
Shousheng Liu ◽  
Zhigang Gai ◽  
Yibao Wang
2000 ◽  
Vol 15 (7) ◽  
pp. 1605-1611 ◽  
Author(s):  
W. H. Guo ◽  
L. F. Chua ◽  
C. C. Leung ◽  
H. W. Kui

When a eutectic melt is undercooled below its liquidus T1 by a critical amount, it undergoes metastable liquid-state spinodal decomposition. The resulting morphologies can be described as intermixing undercooled liquid networks of characteristic wavelength λ. At a temperature substantially below T1, λ can be <100 nm. When λ ≤ 100 nm, the undercooled liquid networks break up into nanometer-size droplets/strips driven apparently by surface tension. The morphologies of the tiny droplets/strips can be frozen by subsequent crystallization. The as-crystallized specimen is a nanostructured material. It is microvoid free and the size of the constituent grains is rather uniform. Two systems, Pd40.5Ni40.5P19 and Pd82Si18, were chosen to illustrate the synthesis process.


2006 ◽  
Vol 294 (1) ◽  
pp. 16-21 ◽  
Author(s):  
Masahito Watanabe ◽  
Kensuke Higuchi ◽  
Akitoshi Mizuno ◽  
Kosuke Nagashio ◽  
Kazuhiko Kuribayashi ◽  
...  

2012 ◽  
Vol 407 (21) ◽  
pp. 4108-4113 ◽  
Author(s):  
Fengxiang Guo ◽  
Ting Lu ◽  
Jingyu Qin ◽  
Hongliang Zheng ◽  
Xuelei Tian

1999 ◽  
Vol 14 (9) ◽  
pp. 3663-3667 ◽  
Author(s):  
K. L. Lee ◽  
H. W. Kui

We demonstrated in “Phase separation in undercooled molten Pd80Si20: Part I” that when a molten Pd80Si20 ingot is undercooled into its undercooling regimen with ΔT ≥ 220 K (ΔT = T1 – T, where T1 is the liquidus and T is the temperature of the undercooled melt), liquid-state phase separation by spinodal decomposition occurs. On crystallization, one of the metastable liquid spinodals becomes Pd3Si, whereas the other one turns into Pd9Si2. In both cases, Pd particles precipitate out. Microstructural analysis indicates the Pd3Si subnetwork forms first. It then acts as a seed for the subsequent crystallization of the remaining undercooled melt, which finally forms the Pd9Si2 dendrites. As crystallization proceeds, latent heat and volume contraction bring about morphological changes.


1997 ◽  
Vol 226-228 ◽  
pp. 434-438 ◽  
Author(s):  
G. Wilde ◽  
S.G. Klose ◽  
W. Soellner ◽  
G.P. Görler ◽  
K. Jeropoulos ◽  
...  

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