Raman scattering as a probe of intermediate phases in glassy networks

被引:43
作者
Boolchand, P. [1 ]
Jin, Mingji [1 ]
Novita, D. I. [1 ]
Chakravarty, S. [1 ]
机构
[1] Univ Cincinnati, Dept Elect & Comp Engn & Comp Sci, Cincinnati, OH 45221 USA
关键词
self-organization in glasses; percolation of rigidity; reversibility window; intermediate phases; raman scattering; photocontraction;
D O I
10.1002/jrs.1707
中图分类号
O433 [光谱学];
学科分类号
0703 ; 070302 ;
摘要
Bulk glass formation occurs over a very small part of phase space, and 'good' glasses (which form even at low quench rates similar to 10 K/sec) select an even smaller part of that accessible phase space. An axiomatic theory provides the physical basis of glass formation, and identifies these sweet spots of glass formation with existence of rigid but stress-free networks for which experimental evidence is rapidly emerging. Recently, theory and experiment have come together to show that these sweet spots of glass formation occur over a range of chemical compositions identified as 'intermediate phases' (IPs). These ranges appear to be controlled by elements of local and medium-range molecular structures that form isostatically rigid networks. IP glasses possess nonhysteretic glass transitions (T-g's) that do not age much. Raman scattering has played a pivotal role in elucidating the molecular structure of glasses in general, and in identifying domains of IPs. Experiments reveal that these phases possess sharp phase boundaries and are characterized by an optical elasticity that varies with network mean coordination number, r, as power law. In this review, we provide examples in chalcogenide and oxide glass systems in which these phases along with optical elasticity power laws have been established. IP glasses represent self-organized nanostructured functional materials optimized by nature. Copyright (c) 2007 John Wiley & Sons, Ltd.
引用
收藏
页码:660 / 672
页数:13
相关论文
共 69 条
[31]   THE NATURE OF THE GLASSY STATE AND THE BEHAVIOR OF LIQUIDS AT LOW TEMPERATURES [J].
KAUZMANN, W .
CHEMICAL REVIEWS, 1948, 43 (02) :219-256
[32]   Quantitative principles of silicate glass chemistry [J].
Kerner, R ;
Phillips, JC .
SOLID STATE COMMUNICATIONS, 2000, 117 (01) :47-51
[33]   On the glass transition temperature in covalent glasses [J].
Kerner, R ;
Micoulaut, M .
JOURNAL OF NON-CRYSTALLINE SOLIDS, 1997, 210 (2-3) :298-305
[34]  
Lagrange J., 1788, MECH ANAL
[35]   RAMAN-SCATTERING AND INFRARED-ABSORPTION IN BULK AMORPHOUS RED PHOSPHORUS [J].
LANNIN, JS ;
SHANABROOK, BV .
SOLID STATE COMMUNICATIONS, 1978, 28 (07) :497-500
[36]   Minimization of dangling bond defects in hydrogenated silicon nitride dielectrics for thin film transistors (TFTs) [J].
Lucovsky, G ;
Phillips, JC .
JOURNAL OF NON-CRYSTALLINE SOLIDS, 1998, 227 :1221-1225
[37]  
LUOCVSKY G, 1977, CTR IND CONSULTANCY, P130
[38]  
Maxwell J. C., 1864, Philosophical Magazine, V27, P294
[39]   Rings and rigidity transitions in network glasses [J].
Micoulaut, M ;
Phillips, JC .
PHYSICAL REVIEW B, 2003, 67 (10) :9
[40]  
MURASE K, 1984, OPTICAL EFFECTS AMOR, P449