7.5.3 Iron-base amorphous alloys

Author(s):  
J. Horváth
Keyword(s):  
1983 ◽  
Vol 25 (9) ◽  
pp. 649-652
Author(s):  
M. A. Drozdova ◽  
A. N. Zhelnov ◽  
A. F. Prokoshin

1979 ◽  
Vol 10 (2-3) ◽  
pp. 294-299 ◽  
Author(s):  
Kazuaki Fukamichi ◽  
Hidetoshi Hiroyoshi ◽  
Michio Kikuchi ◽  
Tsuyoshi Masumoto
Keyword(s):  

1990 ◽  
Vol 32 (3) ◽  
pp. 181-183
Author(s):  
A. N. Novokshonova ◽  
V. V. Pavlov ◽  
I. B. Sobolev ◽  
O. S. Yakushev

1983 ◽  
Vol 25 (9) ◽  
pp. 653-654
Author(s):  
C. P. Pol'dyaeva ◽  
E. K. Zakharov ◽  
V. P. Ovcharov ◽  
B. N. Tret'yakov

ChemInform ◽  
2010 ◽  
Vol 24 (25) ◽  
pp. no-no
Author(s):  
J. CROUSIER ◽  
J. P. CROUSIER ◽  
F. BELLUCCI
Keyword(s):  

1995 ◽  
Vol 10 (4) ◽  
pp. 900-906 ◽  
Author(s):  
Z.H. Lai ◽  
Y.S. Chao ◽  
H. Conrad ◽  
K. Chu

The effects of high current density electropulsing on the hyperfine structure of amorphous alloys Fe73Si9.5B17.5, Fe75Si10B15, and Fe79Si7B14 were investigated by Mössbauer spectroscopy. Electropulsing influenced the microstructure at a temperature well below the bulk crystallization temperature. In the alloy having least boron (or highest concentration of Fe), α-Fe particles ≃3 nm in size precipitated from the amorphous matrix, giving a change in internal magnetic field.


2007 ◽  
Vol 48 (7) ◽  
pp. 1584-1588 ◽  
Author(s):  
Yoon S. Oh ◽  
Hakcheol Lee ◽  
Jung G. Lee ◽  
Nack J. Kim

Author(s):  
A.R. Pelton ◽  
A.F. Marshall ◽  
Y.S. Lee

Amorphous materials are of current interest due to their desirable mechanical, electrical and magnetic properties. Furthermore, crystallizing amorphous alloys provides an avenue for discerning sequential and competitive phases thus allowing access to otherwise inaccessible crystalline structures. Previous studies have shown the benefits of using AEM to determine crystal structures and compositions of partially crystallized alloys. The present paper will discuss the AEM characterization of crystallized Cu-Ti and Ni-Ti amorphous films.Cu60Ti40: The amorphous alloy Cu60Ti40, when continuously heated, forms a simple intermediate, macrocrystalline phase which then transforms to the ordered, equilibrium Cu3Ti2 phase. However, contrary to what one would expect from kinetic considerations, isothermal annealing below the isochronal crystallization temperature results in direct nucleation and growth of Cu3Ti2 from the amorphous matrix.


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