Mechanism of fast surface self-diffusion of an organic glass

被引:55
作者
Capaccioli, S. [1 ,2 ]
Ngai, K. L. [1 ]
Paluch, M. [3 ]
Prevosto, D. [2 ]
机构
[1] Univ Pisa, Phys Dept, I-56127 Pisa, Italy
[2] CNR, IPCF, Inst Chem & Phys Proc, I-56127 Pisa, Italy
[3] Univ Silesia, Inst Phys, PL-40007 Katowice, Poland
来源
PHYSICAL REVIEW E | 2012年 / 86卷 / 05期
关键词
MOLECULAR MOBILITY; POLYMER-FILMS; SECONDARY RELAXATIONS; TRANSITION DYNAMICS; INTERACTING ARRAYS; POLYSTYRENE; FORMERS; INDOMETHACIN; TEMPERATURES; LIQUIDS;
D O I
10.1103/PhysRevE.86.051503
中图分类号
O35 [流体力学]; O53 [等离子体物理学];
学科分类号
070204 ; 080103 ; 080704 ;
摘要
Zhu et al. [L. Zhu, C. W. Brian, S. F. Swallen, P. T. Straus, M. D. Ediger, and L. Yu, Phys. Rev. Lett. 106, 256103 (2011)] measured the surface self-diffusion for an organic glass former, indomethacin, and found surface diffusion is more than 10(6) times faster than bulk diffusion at temperatures around T-g. With the help of dielectric relaxation and differential scanning calorimetry measurements on bulk indomethacin, and analysis of the data using the coupling model, we provide a quantitative explanation. We find the bulk alpha-relaxation time is longer than the primitive relaxation time also by about six orders of magnitude in a range of temperature above and below the bulk T-g. Thus, the cause of the fast surface diffusion is the nearly vanishing of intermolecular coupling of relaxation and diffusion at the surface. The results of related experimental studies of enhanced relaxation and diffusion at the surface of other glass formers also have been analyzed and quantitatively explained. Our predictions on surface diffusion from the coupling model are compared with that given by the random first order transition theory.
引用
收藏
页数:6
相关论文
共 39 条
[11]   Molecular motions of different scales at thin polystyrene film surface by lateral force microscopy [J].
Fu, J ;
Li, BY ;
Han, YC .
JOURNAL OF CHEMICAL PHYSICS, 2005, 123 (06)
[12]   Determination of the viscosity of an amorphous drug using thermomechanical analysis (TMA) [J].
Hancock, BC ;
Dupuis, Y ;
Thibert, R .
PHARMACEUTICAL RESEARCH, 1999, 16 (05) :672-675
[13]   MOLECULAR MOBILITY OF AMORPHOUS PHARMACEUTICAL SOLIDS BELOW THEIR GLASS-TRANSITION TEMPERATURES [J].
HANCOCK, BC ;
SHAMBLIN, SL ;
ZOGRAFI, G .
PHARMACEUTICAL RESEARCH, 1995, 12 (06) :799-806
[14]   Anomalously high-density glass of ethylbenzene prepared by vapor deposition at temperatures close to the glass-transition temperature [J].
Ishii, Kikujiro ;
Nakayama, Hideyuki ;
Hirabayashi, Shin ;
Moriyama, Ryo .
CHEMICAL PHYSICS LETTERS, 2008, 459 (1-6) :109-112
[15]   Dielectric relaxation time of bulk water at 136-140 K, background loss and crystallization effects [J].
Johari, GP .
JOURNAL OF CHEMICAL PHYSICS, 2005, 122 (14)
[16]   SCALING CONCEPTS FOR THE DYNAMICS OF VISCOUS-LIQUIDS NEAR AN IDEAL GLASSY STATE [J].
KIRKPATRICK, TR ;
THIRUMALAI, D ;
WOLYNES, PG .
PHYSICAL REVIEW A, 1989, 40 (02) :1045-1054
[17]   Theory of structural glasses and supercooled liquids [J].
Lubchenko, Vassiliy ;
Wolynes, Peter G. .
ANNUAL REVIEW OF PHYSICAL CHEMISTRY, 2007, 58 :235-266
[18]   Interpreting the dynamics of nano-confined glass-formers and thin polymer films: Importance of starting from a viable theory for the bulk [J].
Ngai, K. L. .
JOURNAL OF POLYMER SCIENCE PART B-POLYMER PHYSICS, 2006, 44 (20) :2980-2995
[19]  
Ngai K. L., 1979, Comments on Solid State Physics, V9, P127
[20]  
Ngai KL, 2011, PART ORDER, P1, DOI 10.1007/978-1-4419-7649-9