Abstract
The Y28 Ti28 Al24 Co20 alloy undergoes metastable liquid phase separation in the under-cooled liquid state and subsequently solidifies into two different Y-rich and Ti-rich amorphous phases. Secondary phase separation occurs due to the supersaturation of the primary separated liquids as the temperature decreases. Depending on the degree of local undercooling, a wide range of length scale of the microstructure is observed. The characteristic length scale of the two amorphous phases is ~250 nm near the air side of the ribbon, and ~25 nm near the wheel side of the ribbon.
| Original language | English |
|---|---|
| Pages (from-to) | 6353-6355 |
| Number of pages | 3 |
| Journal | Applied Physics Letters |
| Volume | 85 |
| Issue number | 26 |
| DOIs | |
| Publication status | Published - 2004 Dec 27 |
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All Science Journal Classification (ASJC) codes
- Physics and Astronomy (miscellaneous)
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In situ formation of two amorphous phases by liquid phase separation in Y-Ti-Al-Co alloy. / Park, B. J.; Chang, H. J.; Kim, D. H.; Kim, W. T.
In: Applied Physics Letters, Vol. 85, No. 26, 27.12.2004, p. 6353-6355.Research output: Contribution to journal › Article
TY - JOUR
T1 - In situ formation of two amorphous phases by liquid phase separation in Y-Ti-Al-Co alloy
AU - Park, B. J.
AU - Chang, H. J.
AU - Kim, D. H.
AU - Kim, W. T.
PY - 2004/12/27
Y1 - 2004/12/27
N2 - The Y28 Ti28 Al24 Co20 alloy undergoes metastable liquid phase separation in the under-cooled liquid state and subsequently solidifies into two different Y-rich and Ti-rich amorphous phases. Secondary phase separation occurs due to the supersaturation of the primary separated liquids as the temperature decreases. Depending on the degree of local undercooling, a wide range of length scale of the microstructure is observed. The characteristic length scale of the two amorphous phases is ~250 nm near the air side of the ribbon, and ~25 nm near the wheel side of the ribbon.
AB - The Y28 Ti28 Al24 Co20 alloy undergoes metastable liquid phase separation in the under-cooled liquid state and subsequently solidifies into two different Y-rich and Ti-rich amorphous phases. Secondary phase separation occurs due to the supersaturation of the primary separated liquids as the temperature decreases. Depending on the degree of local undercooling, a wide range of length scale of the microstructure is observed. The characteristic length scale of the two amorphous phases is ~250 nm near the air side of the ribbon, and ~25 nm near the wheel side of the ribbon.
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UR - http://www.scopus.com/inward/citedby.url?scp=13444293108&partnerID=8YFLogxK
U2 - 10.1063/1.1842360
DO - 10.1063/1.1842360
M3 - Article
AN - SCOPUS:13444293108
VL - 85
SP - 6353
EP - 6355
JO - Applied Physics Letters
JF - Applied Physics Letters
SN - 0003-6951
IS - 26
ER -