Related Experiment Videos
Freezing of dynamical exponents in low dimensional random media.
1CNRS-Laboratoire de Physique Théorique de l'Ecole Normale Supérieure, 24 rue Lhomond, 75231 Cedex 05, Paris, France.
Physical Review Letters
|June 1, 2001
Summary
A particle in a random potential exhibits a dynamical transition at a finite temperature. This transition, relevant to glass phases and dislocation motion, involves barriers and valleys in one dimension.
Area of Science:
- Condensed matter physics
- Statistical mechanics
- Disordered systems
Background:
- Understanding the behavior of particles in random potentials is crucial for various fields.
- The study of dynamical transitions and glass phases is a complex area in physics.
Purpose of the Study:
- To investigate the dynamical transition of a particle in a random potential with logarithmic correlations in dimensions d=1,2.
- To analyze the relationship between static and dynamic properties in disordered systems.
Main Methods:
- Exact results in d=1 for the dynamical transition temperature and dynamical exponent.
- Analytical arguments for d=2, extending findings to related systems like the 2D random gauge XY model.
- Analysis of freezing mechanisms involving energy barriers and valleys.
Main Results:
- A dynamical transition occurs at a positive temperature T(dyn)>0.
- In d=1, T(dyn) equals the static glass transition temperature T(c).
- The dynamical exponent z(T) exhibits distinct behaviors in high-temperature and glass phases, with similar formulas proposed for d=2.
Conclusions:
- Dynamical freezing is predicted in the studied systems, including the 2D random gauge XY model.
- In d=1, a mapping between dynamics and statics reveals freezing involves both barriers and valleys.
- Anomalous scaling in creep dynamics has implications for understanding dislocation motion.