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Overview
• We study a short-ranged attractive system in the reentrant region of the glass phase diagram
• We quench the system deep in the glass by lowering and increasing the temperature
• The aging properties of this two states have been studied by molecular dynamics
The numerical experiment
• We prepared 60 independent configurations equilibrated at T=0.6
• We quenched the system at two point state:
T=1.2 in the repulsive glass T=0.3 in the attractive glass
• After that the system evolves at constant temperature.
AgingWe are studying an out-of-equilibrium process!
• Time translational invariance does not hold
• One time observable (i.g. energy and static structure factors) will depend on the waiting time
• Correlation function will depend on the observation time and the waiting time:
Energy evolution
• After the quench the system present two different evolution of the energy:– @T=1.2 the energy
increase and can be fitted with a log.
– @T=0.3 the energy decrease and follows a power law:
Static structure factors
• The overall shape of the S(q) does not change with a waiting time
• Only a slightly increase (decrease) in the first peak is present
Scaling Theoretical studies (Cugliandolo cond-mat/0210312) suggest the possibility of rescaling the correlators ad different waiting time
For example:
Simple aging case
Proposed for BMLJ with 0.88 [1]
[1] Kob and Barrat PRL 78, 4581 (1997)
Scaling for the attractive glass
Even if the scaling time can be fitted with a power law (with approx. 0.38) the collapse of the correlators into a master curve is not satisfactory.
Mean Squared Displacement
@T=1.2
There is a clear plateau that grows with the waiting time
@T=0.3
There is no clear plateau but rather a power law increase in that follows a power law (with an exponent that grows with waiting time)
Conclusion
The repulsive and the attractive glasses aging scenario has been numerically investigated
• Static structure factors do not change significantly with time
• Density-density correlation functions evolves with the waiting time in a completely different way
• No scaling properties with waiting time• Good agreement with experimental results.