L-1

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 Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle N } spins Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \sigma_i=\pm 1} and i.i.d. coupling Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle J_{ij} } drawn from a distribution $\pi(J)$. 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 <\math><\center>

\overline{J_{ij}}=0 

</math>

Hence the energy associated to a given configuration Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \sigma_i=\pm 1}

 with zero average.

The For simplicity we assume <\math>

H= \sum_{ i j } J_{ij} \sigma_i \sigma_j

</math>