The optical, electrical, and magnetic properties of alkali metal amine solutions

1976 ◽  
Vol 80 (19) ◽  
pp. 2117-2123 ◽  
Author(s):  
S. Nehari ◽  
K. Bar-Eli
1964 ◽  
Vol 40 (12) ◽  
pp. 3729-3730 ◽  
Author(s):  
Michael Ottolenghi ◽  
Kedma Bar‐Eli ◽  
Henry Linschitz ◽  
T. R. Tuttle

1973 ◽  
Vol 77 (3) ◽  
pp. 323-325 ◽  
Author(s):  
K. Bar-Eli ◽  
G. Gabor

1957 ◽  
Vol 0 (0) ◽  
pp. 3329-3336 ◽  
Author(s):  
G. W. A. Fowles ◽  
W. R. McGregor ◽  
M. C. R. Symons

1970 ◽  
Vol 74 (17) ◽  
pp. 3285-3290 ◽  
Author(s):  
D. Huppert ◽  
Kedma H. Bar-Eli

1968 ◽  
Vol 48 (6) ◽  
pp. 2818-2819 ◽  
Author(s):  
Ian Hurley ◽  
T. R. Tuttle ◽  
Sidney Golden

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.


2018 ◽  
Vol 44 (7) ◽  
pp. 595-598 ◽  
Author(s):  
V. V. Balashev ◽  
K. S. Ermakov ◽  
L. A. Chebotkevich ◽  
V. V. Korobtsov

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