Abstract
The development of order for the Ising model in the presence of static, random impurities is studied following a quench from high temperature (TTc) to T<Tc. We find that for quenches to T=0, the system becomes pinned for long times for any value of c>0 and never reaches its final equilibrium ferromagnetic ground state. The average linear pinned domain size scales as the inverse square root of the concentration c. For quenches to a final T>0, the long-time behavior of the correlation length R and the energy E are slower than a power law, suggesting a logarithmic growth law for long times. The time that is required to reach this asymptotic logarithmic behavior increases as the impurity concentration decreases and/or the temperature increases. © 1985 The American Physical Society.
| Original language | English |
|---|---|
| Pages (from-to) | 3014-3020 |
| Number of pages | 7 |
| Journal | Physical Review B |
| Volume | 32 |
| Issue number | 5 |
| DOIs | |
| State | Published - Jan 1 1985 |
| Externally published | Yes |
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