Formation and Properties of Amorphous and Nanocrystalline Phases in Mechanically Alloyed Fe-Based Multicomponent Alloys
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		    determined using the well-known Scherrer formula. Due to wear debris of the milling tools, chemical analysis of the milled powders revealed a slight increase of the Fe content (< 0.8 at.% Fe) compared to the nominal composition of the alloys. Thermal analysis was done in a PerkinElmer DSC 7 and TMA 7 at heating rates of 10 and 40 K/min. RESULTS AND DISCUSSION
 
 Figure 1 shows x-ray diffraction patterns for
 
 Fe 72 (A15 PIIC 6 B 4 )1 +2/26
 
 after different milling
 
 times as a typical example. With increasing processing time a decrease of the crystalline Fe and Al diffraction peaks and the formation of a broad diffuse diffraction intensity corresponding to an amorphous phase can be seen. In addition, a broadening of the bcc Fe lines due to a decreasing grain size and an increase in atomic-level strain is observed. In contrast to singlephase amorphous ribbons produced by rapid quenching [3, 4], mechanical alloying of elemental powders reveals an additional nanoscale bcc Fe-rich phase after 130 h of milling. For the initially quaternary Fe 7 9P1 IC 6B 4 alloy and a substitution of Fe by 5 at.% Al (Fe74A15 PI 1C6 B4 ) and 2 at.% Ga (Fe72Al 5PJ 1C6B4Ga 2) the formation of an amorphous/nanocrystalline phase mixture is
 
 obtained (Fig. 2). Figure 3 shows x-ray diffraction patterns for
 
 Fe74 -x(Al5Pi 1C 6 B4 )1 1+x26
 
 with
 
 different composition. This change in composition was chosen to maintain a fixed A15 PIIC 6B4 ratio. Starting with Fe 74A15PI IC6B4 a change of the Fe content in Fe 74_x(Al 5 PH C 6B 4)i+x/26 (x = 2, 4, 5, 6) also leads to an amorphous/nanocrystalline phase mixture after a milling time of 130 h for all compositions. Using the well-known Scherrer formula, the average grain size was estimated from the full-width at half maximum (FWHM) of the Fe reflections after correction for instrumental broadening. For all samples investigated a grain size of 10 ± 2 nm was found.
 
 C6
 
 --3
 
 *
 
 Cu
 
 o Al
 
 Fe
 
 Cu
 
 co
 
 U'Ul) C
 
 t'-
 
 =2h m
 
 -
 
 20
 
 Figure 1:
 
 40
 
 60 80 100 2 0 [degrees]
 
 120
 
 40
 
 X-ray diffraction patterns for
 
 Fe7 2(A15P 11C 6 B4 )1+2/26 after
 
 St
 
 50
 
 60 70 80 90 100 110 2 0 [degrees]
 
 Figure 2: X-ray diffraction patterns for Fe 79P11C 6 B 4 , Fe74AA5P1 IC6B 4 and Fe 72 A15P[ IC6 B4 Ga 2 after 130 h of milling.
 
 different milling
 
 times.
 
 508
 
 Fe.
 
 (AIP
 
 CB.)
 
 tm= 130h
 
 t = 130h
 
 74-x" 5 11 6 4 1+x/26 x =2 mx=2Tj
 
 Fe
 
 -
 
 P GB
 
 T
 
 79 11 6 4
 
 Cd
 
 T
 
 xx=4
 
 o
 
 M
 
 Fe Al5P C6B4Ga
 
 -
 
 64
 
 72 511
 
 [Z
 
 x
 
 2
 
 X=5x 0
 
 FeFAIsP1C B 4
 
 E x 6
 
 50
 
 60
 
 70
 
 80
 
 90
 
 T
 
 4
 
 x
 
 X
 
 -
 
 40
 
 74 5 11 6 4
 
 ILl
 
 100
 
 640
 
 110
 
 2 0 [degrees]
 
 680
 
 720
 
 760
 
 800
 
 Temperature [ K]
 
 Figure 3: X-ray diffraction patterns for Fe 74 _x(A15P1 lC 6B4 )1 +,/ 26 after 130 h of milling.
 
 Figure 4: DSC scans (heating rate 40 K/min) for Fe 79 P11 C6 B 4 , Fe 72A15 PIIC 6B4 Ga 2 and Fe 74A15PIIC 6B 4 after 130 h of milling.
 
 The thermal stability of the milled powders was investigated by DSC. All samples exhibit an endothermic event reflecting the heat capacity anomaly characteristic of the glass transition and a sharp exothermic reaction at higher tem		
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