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- transition to a ``glassy'' phase at low temperatures
- susceptibility has a cusp rather than a divergence at
- very large number of metastable states (local minimum of energy) in spin
glass phase
- long equilibration times (logarithmic rather than exponential relaxation
to equilibrium) --- remanent magnetization
- degeneracy (or near-degeneracy) of ground state, with many
configurations having (nearly) the lowest energy value
- finding ground states is a difficult (NP hard) problem
- main properties of real spin glasses (e.g. amorphous alloys)
can be described fairly well by
spin
glass Ising model on a regular crystalline lattice
Paul Coddington, Northeast Parallel Architectures Center at Syracuse University, paulc@npac.syr.edu