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Existence of the Free Energy and Self-Averaging

This section is devoted to the proof of the existence of the quenched free energy. The free energy of a disordered system is a priori a random variable, however we will show that it is a degenerate random variable, i.e. a constant this phenomenon is called self-averaging property of the free energy. [Pg.90]

The first step in the proof is controlling the so-caUed quenched averaged free energy by the bound on Hn,u(t) in point (1) in Section 4.1, and by the hypothesis on cu, logZ L. As a matter of fact the same bound implies directly [Pg.90]

So that the sequence with which we wish to define, in the limit, the quenched averaged free energy is bounded above. By using the same esti- [Pg.90]

By taking the P-expectation, keeping in mind that logZ log coincide in law, we obtain the statement. [Pg.91]

Combining Proposition 4.2 and Proposition A.12 the existence of the limit of the sequence ElogZ is established and we set [Pg.91]


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