In recent years, much experimental and numerical evidence has been accumulated for the existence of liquid-liquid structure changes induced by temperature or pressure. [1][2][3] Lots of work have proved that the melt temperature could change glass forming ability (GFA), thermal stability, and mechanical properties of a metallic glass. [4][5][6] Recently, the liquid-liquid structure transition (LLST) has been found in Zr-based metallic glass formers by Li et al. using electrostatic levitation. They also found that the LLST influenced the crystallization behavior of the metallic glasses. [7] For Al-based alloys, the viscosity and surface tension of Al 91 La 5 Ni 4 and Al 91 Ce 5 Ni 4 melts indicated that an irreversible atomic redistribution existed in the melts. [8,9] X-ray diffraction (XRD) experiments showed that there was abrupt change in the pair correlation function g(r) of the Al 85 Ni 10 Ce 5 alloy in the range from 1270 to 1480 K. [10] It suggested that some Al-TM-RE alloys may also exhibit LLST behavior.Aluminum-based Al-TM-RE (TM-transition metals, RE-rare earth elements) amorphous alloys with high Al contents (>80 at%) exhibit high strength in combination with good ductility and corrosion, which makes them suitable for application as structural materials. [11,12] Therefore, the GFA as well as the crystallization process of the Al-based amorphous alloys has been drawn much attention. However, little attention has been paid to the influence of the LLST on the GFA and the crystallization behavior of Al-based amorphous alloys. In the present work, the variations of electrical resistivity (ER) and differential thermal analysis (DTA) as a function of temperature for the Al 86 Ni 9 La 5[13] melt were investigated by continuous heating. Based on the anomalous behavior of LLST observed in the melt, three melt temperatures were chosen to prepare the amorphous samples and then the effects of quenching temperature on the GFA and the crystallization behavior were studied.
ExperimentalThe Al 86 Ni 9 La 5 alloy ingots were prepared by arc melting the mixtures of pure Al (99.999%), Ni (99.99%), and La (99.9%) metals in a titanium-gettered argon atmosphere in a watercooled copper crucible. The ingots were remelted six times to ensure compositional homogeneity and then were divided into three pieces. One of them was remelted and then suction casting into a copper mold to obtain F5 Â 50 mm 3 cylindrical rods for ER measurement. The ER against temperature was measured using the D. C. four-probe method under vacuum of about 10 À2 Pa. The continuous heating process of the alloy was measured using a DTA instrument at a heating rate of 10 K min À1 . Another ingot pieces were then ejected into a wedge-shaped copper mold with an inclined angle of 58 and 10 mm in width. According to the LLST observed by both ER and DTA measurement, three quenching temperatures were chosen to prepare wedge-shaped samples according to the temperature with the anomalous changes of ER, which were During the heating process the temperature-induced liq...