Abstract
The dynamic mean field theory of the spin glass phase is generalised to n-component spins. Exact averaged equations of motion are derived within a purely relaxational model. It is shown that dynamic stability enforces a violation of the fluctuation-dissipation theorem for any finite n and T<Tc. The marginally stable state is characterised by algebraic decay of correlations t- nu with an exponent which depends continuously on temperature and the number of components, nu (T,n)= 1/2-3 mod T-Tc mod / pi n(n+2)+O( mod T-T c mod 2)+O(1/n3).
Original language | English |
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Article number | 003 |
Pages (from-to) | L1059-L1064 |
Journal | Journal of Physics C: Solid State Physics |
Volume | 15 |
Issue number | 30 |
DOIs | |
State | Published - 1982 |
Externally published | Yes |