2019
DOI: 10.1016/j.intermet.2019.03.007
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Preparation of bulk metallic glasses by modifying local structure of icosahedral quasicrystals

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Cited by 8 publications
(3 citation statements)
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“…Figures 1(c quasi-crystals are the main competing phase against noncrystals, higher difficulty in crystallization of quasi-crystals indicates a higher glass formability. This result was in line with the earlier reported study [30] in that, with the increased Be content, the critical glassy size increases from 2 mm for the alloy Be20%, to 15 mm for the alloy Be24%, to the peak value of 20 mm for the alloy Be28%, and then drops to 12 mm for alloy Be32%.…”
Section: Experimental Worksupporting
confidence: 93%
See 1 more Smart Citation
“…Figures 1(c quasi-crystals are the main competing phase against noncrystals, higher difficulty in crystallization of quasi-crystals indicates a higher glass formability. This result was in line with the earlier reported study [30] in that, with the increased Be content, the critical glassy size increases from 2 mm for the alloy Be20%, to 15 mm for the alloy Be24%, to the peak value of 20 mm for the alloy Be28%, and then drops to 12 mm for alloy Be32%.…”
Section: Experimental Worksupporting
confidence: 93%
“…As described in our earlier studies, [30] homogeneous ingots of (Zr 40 Ti 40 Ni 20 ) 100−x Be x (x = 0, 20, 24, 28, 32) were prepared by melting mixtures of high-purity elements (>99.9 wt%) five times under an Ar atmosphere in an arc-melting furnace. The copper mold suction casting method was used to prepare alloy rods with different sizes.…”
Section: Experimental Workmentioning
confidence: 99%
“…[ 53 ] Moreover, based on the metallic compounds of low Δ S m , glassy materials have been successfully designed and prepared such as a semiconductor glass of Ga 2 Te 3 ‐SnTe [ 54 ] and bulk metallic glasses of (Zr 40 Ti 40 Ni 20 ) 100‐x Be x . [ 55 ] Theoretically, the Gibbs free energy difference Δ G l‐s between liquid and solid phases is associated with glass formation due to its nature of the crystallization driving force. Δ G l‐s can be expressed in terms of [ 13 ] Δ G l − s = Δ S m Δ T + f (Δ T ), where Δ T is the degree of supercooling relative to T m , and f (Δ T ) is the higher‐order function.…”
Section: Discussionmentioning
confidence: 99%