Fast and slow crystal growth kinetics in glass-forming melts

被引:100
作者
Orava, J.
Greer, A. L. [1 ]
机构
[1] Tohoku Univ, WPI AIMR, Aoba Ku, 2-1-1 Katahira, Sendai, Miyagi 9808577, Japan
关键词
PHASE-CHANGE MATERIALS; LIQUID-METALS; VISCOSITY; CRYSTALLIZATION; SOLIDIFICATION; TEMPERATURE; NUCLEATION; TRANSITION; DIFFUSION; SELENIUM;
D O I
10.1063/1.4880959
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
Published values of crystal growth rates are compared for supercooled glass-forming liquids undergoing congruent freezing at a planar crystal-liquid interface. For the purposes of comparison pure metals are considered to be glass-forming systems, using data from molecular-dynamics simulations. For each system, the growth rate has a maximum value U-max at a temperature T-max that lies between the glass-transition temperature T-g and the melting temperature T-m. A classification is suggested, based on the lability (specifically, the propensity for fast crystallization), of the liquid. High-lability systems show "fast" growth characterized by a high U-max, a low T-max/T-m, and a very broad peak in U vs. T/T-m. In contrast, systems showing "slow" growth have a low Umax, a high T-max/T-m, and a sharp peak in U vs. T/T-m. Despite the difference of more than 11 orders of magnitude in U-max seen in pure metals and in silica, the range of glass-forming systems surveyed fit into a common pattern in which the lability increases with lower reduced glass-transition temperature (T-g/T-m) and higher fragility of the liquid. A single parameter, a linear combination of T-g/T-m and fragility, can show a good correlation with U-max. For all the systems, growth at Umax is coupled to the atomic/molecular mobility in the liquid. It is found that, across the diversity of glass-forming systems, T-max/T-g = 1.48 +/- 0.15. (C) 2014 AIP Publishing LLC.
引用
收藏
页数:10
相关论文
共 55 条
[1]   Kinetic coefficient for hard-sphere crystal growth from the melt [J].
Amini, Majeed ;
Laird, Brian B. .
PHYSICAL REVIEW LETTERS, 2006, 97 (21)
[2]   Crystal nucleation and growth of indomethacin polymorphs from the amorphous state [J].
Andronis, V ;
Zografi, G .
JOURNAL OF NON-CRYSTALLINE SOLIDS, 2000, 271 (03) :236-248
[3]  
Angell C.A., 1985, RELAXATIONS COMPLEX
[4]   FORMATION OF GLASSES FROM LIQUIDS AND BIOPOLYMERS [J].
ANGELL, CA .
SCIENCE, 1995, 267 (5206) :1924-1935
[5]   Kinetic stages in the crystallization of deeply undercooled body-centered-cubic and face-centered-cubic metals [J].
Ashkenazy, Y. ;
Averback, R. S. .
ACTA MATERIALIA, 2010, 58 (02) :524-530
[6]   THE VISCOSITY OF LIQUID-METALS AND ALLOYS [J].
BATTEZZATI, L ;
GREER, AL .
ACTA METALLURGICA, 1989, 37 (07) :1791-1802
[7]   Characterization of the molecular structure of amorphous selenium using recoverable creep compliance measurements [J].
Bernatz, KM ;
Echeverría, I ;
Simon, SL ;
Plazek, DJ .
JOURNAL OF NON-CRYSTALLINE SOLIDS, 2002, 307 :790-801
[8]   Review of data for velocity of sound in pure liquid metals and metalloids [J].
Blairs, S. .
INTERNATIONAL MATERIALS REVIEWS, 2007, 52 (06) :321-344
[9]   CRYSTALLIZATION RATES OF A LENNARD-JONES LIQUID [J].
BROUGHTON, JQ ;
GILMER, GH ;
JACKSON, KA .
PHYSICAL REVIEW LETTERS, 1982, 49 (20) :1496-1500
[10]   Observation and modeling of polycrystalline grain formation in Ge2Sb2Te5 [J].
Burr, Geoffrey W. ;
Tchoulfian, Pierre ;
Topuria, Teya ;
Nyffeler, Clemens ;
Virwani, Kumar ;
Padilla, Alvaro ;
Shelby, Robert M. ;
Eskandari, Mona ;
Jackson, Bryan ;
Lee, Bong-Sub .
JOURNAL OF APPLIED PHYSICS, 2012, 111 (10)