Abstract
If liquids, polymers, bio-materials, metals and molten salts can avoid crystallization during cooling or compression, they freeze into a microscopically disordered solid-like state, a glass1,2. On approaching the glass transition, particles become trapped in transient cages—in which they rattle on picosecond timescales—formed by their nearest neighbours; the particles spend increasing amounts of time in their cages as the average escape time, or structural relaxation time τα, increases from a few picoseconds to thousands of seconds through the transition. Owing to the huge difference between relaxation and vibrational timescales, theoretical3,4,5,6,7,8,9 studies addressing the underlying rattling process have challenged our understanding of the structural relaxation. Numerical10,11,12,13 and experimental studies on liquids14 and glasses8,15,16,17,18,19 support the theories, but not without controversies20 (for a review see ref. 21). Here we show computer simulations that, when compared with experiments, reveal the universal correlation of the structural relaxation time (as well as the viscosity η) and the rattling amplitude from glassy to low-viscosity states. According to the emerging picture the glass softens when the rattling amplitude exceeds a critical value, in agreement with the Lindemann criterion for the melting of crystalline solids22 and the free-volume model23.
This is a preview of subscription content, access via your institution
Access options
Subscribe to this journal
Receive 12 print issues and online access
$259.00 per year
only $21.58 per issue
Buy this article
- Purchase on SpringerLink
- Instant access to the full article PDF.
USD 39.95
Prices may be subject to local taxes which are calculated during checkout


.
Similar content being viewed by others
References
Angell, C. A. Relaxation in liquids, polymers and plastic crystals—strong/fragile patterns and problems. J. Non-Cryst. Solids 131–133, 13–31 (1991).
Debenedetti, P. G. & Stillinger, F. H. Supercooled liquids and the glass transition. Nature 410, 259–267 (2001).
Tobolsky, A., Powell, R. E. & Eyring, H. in Frontiers in Chemistry Vol. 1 (eds Burk, R. E. & Grummit, O.) 125–190 (Interscience, New York, 1943).
Angell, C. A. Formation of glasses from liquids and biopolymers. Science 267, 1924–1935 (1995).
Hall, R. W. & Wolynes, P. G. The aperiodic crystal picture and free energy barriers in glasses. J. Chem. Phys. 86, 2943–2948 (1987).
Dyre, J. C., Olsen, N. B. & Christensen, T. Local elastic expansion model for viscous-flow activation energies of glass-forming molecular liquids. Phys. Rev. B 53, 2171–2174 (1996).
Ngai, K. L. Dynamic and thermodynamic properties of glass-forming substances. J. Non-Cryst. Solids 275, 7–51 (2000).
Martinez, L.-M. & Angell, C. A. A thermodynamic connection to the fragility of glass-forming liquids. Nature 410, 663–667 (2001).
Ngai, K. L. Why the fast relaxation in the picosecond to nanosecond time range can sense the glass transition. Phil. Mag. 84, 1341–1353 (2004).
Shao, J. & Angell, C. A. Proc. XVIIth International Congress on Glass, Beijing Vol. 1, 311–320 (Chinese Ceramic Society, Beijing, 1995).
Starr, F. W., Sastry, S., Douglas, J. F. & Glotzer, S. What do we learn from the local geometry of glass-forming liquids? Phys. Rev. Lett. 89, 125501 (2002).
Bordat, P., Affouard, F., Descamps, M. & Ngai, K. L. Does the interaction potential determine both the fragility of a liquid and the vibrational properties of its glassy state? Phys. Rev. Lett. 93, 105502 (2004).
Widmer-Cooper, A. & Harrowell, P. Predicting the long-time dynamic heterogeneity in a supercooled liquid on the basis of short-time heterogeneities. Phys. Rev. Lett. 96, 185701 (2006).
Buchenau, U. & Zorn, R. A relation between fast and slow motions in glassy and liquid selenium. Europhys. Lett. 18, 523–528 (1992).
Sokolov, A. P., Rössler, E., Kisliuk, A. & Quitmann, D. Dynamics of strong and fragile glass formers: Differences and correlation with low-temperature properties. Phys. Rev. Lett. 71, 2062–2065 (1993).
Scopigno, T., Ruocco, G., Sette, F. & Monaco, G. Is the fragility of a liquid embedded in the properties of its glass? Science 302, 849–852 (2003).
Buchenau, U. & Wischnewski, A. Fragility and compressibility at the glass transition. Phys. Rev. B 70, 092201 (2004).
Novikov, V. N. & Sokolov, A. P. Poisson’s ratio and the fragility of glass-forming liquids. Nature 431, 961–963 (2004).
Novikov, V. N., Ding, Y. & Sokolov, A. P. Correlation of fragility of supercooled liquids with elastic properties of glasses. Phys. Rev. E 71, 061501 (2005).
Yannopoulos, S. N. & Johari, G. P. Poisson’s ratio and liquid’s fragility. Nature 442, E7–E8 (2006).
Dyre, J. C. The glass transition and elastic models of glass-forming liquids. Rev. Mod. Phys. 78, 953–972 (2006).
Löwen, H. Melting, freezing and colloidal suspensions. Phys. Rep. 237, 249–324 (1994).
Gedde, U. W. Polymer Physics (Chapman and Hall, London, 1995).
Xia, X. & Wolynes, P. G. Fragilities of liquids predicted from the random first order transition theory of glasses. Proc. Natl Acad. Sci. 97, 2990–2994 (2000).
Bässler, H. Viscous flow in supercooled liquids analyzed in terms of transport theory for random media with energetic disorder. Phys. Rev. Lett. 58, 767–770 (1987).
Ferry, J. D., Grandine, L. D. Jr & Fitzgerald, E. R. The relaxation distribution function of polyisobutylene in the transition from rubber-like to glass-like behavior. J. Appl. Phys. 24, 911–916 (1953).
Monthus, C. & Bouchaud, J.-P. Models of traps and glass phenomenology. J. Phys. A 29, 3847–3869 (1996).
Kröger, M. Simple models for complex nonequilibrium fluids. Phys. Rep. 390, 453–551 (2004).
Boon, J. P. & Yip, S. Molecular Hydrodynamics (Dover, New York, 1980).
Glotzer, S. C. & Vogel, M. Temperature dependence of spatially heterogeneous dynamics in a model of viscous silica. Phys. Rev. E 70, 061504 (2004).
Acknowledgements
The authors acknowledge discussions with C. A. Angell, S. Capaccioli, G. Carini, P. G. Debenedetti, J. Dyre, A. Fontana, K. L. Ngai, G. Ruocco, F. Sciortino and S. N. Shore. A. Wischnewski is thanked for providing the DW data of silica. Computational resources by ‘Laboratorio per il Calcolo Scientifico’ (Physics Department, University of Pisa) and financial support from MIUR within the PRIN project ‘Aging, fluctuation and response in out-of-equilibrium glassy systems’ are acknowledged.
Author information
Authors and Affiliations
Corresponding author
Supplementary information
Supplementary Information
Simulations and Experimental data and scaling (PDF 139 kb)
Rights and permissions
About this article
Cite this article
Larini, L., Ottochian, A., De Michele, C. et al. Universal scaling between structural relaxation and vibrational dynamics in glass-forming liquids and polymers. Nature Phys 4, 42–45 (2008). https://doi.org/10.1038/nphys788
Received:
Accepted:
Published:
Issue date:
DOI: https://doi.org/10.1038/nphys788
This article is cited by
-
Direction-dependent dynamics of colloidal particle pairs and the Stokes-Einstein relation in quasi-two-dimensional fluids
Nature Communications (2023)
-
Thermal expansion and the glass transition
Nature Physics (2023)
-
A Thermodynamic Perspective on Polymer Glass Formation
Chinese Journal of Polymer Science (2023)
-
Origin of the boson peak in amorphous solids
Nature Physics (2022)
-
Systematic coarse-graining of epoxy resins with machine learning-informed energy renormalization
npj Computational Materials (2021)


