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We indicate the avergage over the couplings (namely the average over the disorder) with an overline. In this case we have | We indicate the avergage over the couplings (namely the average over the disorder) with an overline. In this case we have | ||
<center><math> | <center><math> | ||
\ | \bar{J_{ij}}=0 | ||
</math></center> | </math></center> | ||
Hence the energy associated to a given configuration <math> \sigma_i=\pm 1</math> | Hence the energy associated to a given configuration <math> \sigma_i=\pm 1</math> | ||
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The | The | ||
For simplicity we assume | For simplicity we assume | ||
< | <center> <math> | ||
H= \sum_{ i j } J_{ij} \sigma_i \sigma_j | H= \sum_{ i j } J_{ij} \sigma_i \sigma_j | ||
</math></center> | </math></center> |
Revision as of 15:17, 12 November 2023
Spin glass Transition
Experiments
Parlare dei campioni di rame dopati con il magnesio, marino o no: trovare due figure una di suscettivita e una di calore specifico, prova della transizione termodinamica.
Edwards Anderson model
We consider an Ising model with spins and i.i.d. coupling drawn from a distribution . It is crucial to assume that the mean value of the couplings is zero, otherwise the model displays ferro/antiferro order. We indicate the avergage over the couplings (namely the average over the disorder) with an overline. In this case we have
Hence the energy associated to a given configuration
with zero average.
The For simplicity we assume