Four-point susceptibility of a glass-forming binary mixture: Brownian dynamics

Physical Review E - Statistical, Nonlinear, and Soft Matter Physics

Volumn 74, Issue 2, 2006, Pages

  Szamel, Grzegorz ^a   Flenner, Elijah ^a  

^a Department of Environmental and Radiological Health Sciences   (United States)

Author keywords

[No Author keywords available]

Indexed keywords

BROWNIAN MOVEMENT; COMPUTER SIMULATION; GLASS; STATISTICAL MECHANICS;

BROWNIAN DYNAMICS; KOB-ANDERSEN LENNARD-JONES MIXTURE; QUALITATIVE PREDICTIONS;

BINARY MIXTURES;

EID: 33747137648     PISSN: 15393755     EISSN: 15502376     Source Type: Journal    
DOI: 10.1103/PhysRevE.74.021507     Document Type: Article

References (21)

1. See, e.g., P. G. Debenedettin and F. H. Stillinger, Nature (London) NATUAS 0028-0836 10.1038/35065704 410, 259 (2001).
2. J.-P. Bouchaud and G. Biroli, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.72.064204 72, 064204 (2005).
3. C. Toninelli, M. Wyart, L. Berthier, G. Biroli, and J.-P. Bouchaud, Phys. Rev. E PLEEE8 1063-651X 10.1103/PhysRevE.71.041505 71, 041505 (2005).
4. L. Berthier, G. Biroli, J.-P. Bouchaud, L. Cipelletti, D. El Masri, D. LâHote, F. Ladieu, and M. Pierno, Science SCIEAS 0036-8075 10.1126/science.1120714 310, 1797 (2005).
5. W. Kob and H. C. Andersen, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.73.1376 73, 1376 (1994);
6. W. Kob and H. C. Andersen, Phys. Rev. E PLEEE8 1063-651X 10.1103/PhysRevE.51.4626 51, 4626 (1995);
7. W. Kob and H. C. Andersen, Phys. Rev. E PLEEE8 1063-651X 10.1103/PhysRevE.52.4134 52, 4134 (1995).
8. The alternative used in other stochastic dynamics simulations is to explicitly modify the noise in such a way that the center of mass does not move [W. Kob (private communication)].
9. S. Franz, C. Donati, G. Parisi, and S. C. Glotzer, Philos. Mag. B PMABDJ 1364-2812 10.1080/014186399255953 79, 1827 (1999);
10. C. Donati, S. Franz, S. C. Glotzer, and G. Parisi, J. Non-Cryst. Solids JNCSBJ 0022-3093 10.1016/S0022-3093(02)01461-8 307, 215 (2002);
11. S. C. Glotzer, V. N. Novikov, and T. B. Schrøder, J. Chem. Phys. JCPSA6 0021-9606 10.1063/1.480541 112, 509 (2000).
12. Recently a cond-mat report was posted (D. Chandler, J. P. Garrahan, R. L. Jack, L. Maibaum, A. C. Pan, eprint cond-mat/0605084) which discusses the dependence of the four-point susceptibility χ kâ- (t) on the magnitude of the wave vector kâ-.
13. W. GÃtze, in Liquids, Freezing and Glass Transition, edited by, J. P. Hansen, D. Levesque, and, J. Zinn-Justin, (North-Holland, Amsterdam, 1991).
14. G. Szamel and H. LÃwen, Phys. Rev. A PLRAAN 1050-2947 10.1103/PhysRevA.44.8215 44, 8215 (1991).
15. G. Biroli and J.-P. Bouchaud, Europhys. Lett. EULEEJ 0295-5075 10.1209/epl/i2003-10156-5 67, 21 (2004).
16. L. Berthier and G. Biroli (private communication).
17. E. Flenner and G. Szamel, Phys. Rev. E PLEEE8 1063-651X 10.1103/PhysRevE.72.031508 72, 031508 (2005).
18. J. P. Garrahan and D. Chandler, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.89.035704 89, 035704 (2002);
19. J. P. Garrahan and D. Chandler, Proc. Natl. Acad. Sci. U.S.A. PNASA6 0027-8424 10.1073/pnas.1233719100 100, 9710 (2003).
20. L. Berthier and J. P. Garrahan, J. Chem. Phys. JCPSA6 0021-9606 10.1063/1.1593020 119, 4367 (2003);
21. L. Berthier and J. P. Garrahan, Phys. Rev. E PLEEE8 1063-651X 10.1103/PhysRevE.68.041201 68, 041201 (2003).