TBan-I: Difference between revisions

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<center><math> \overline{n(x)} = M (M-1) \int_{-\infty}^\infty dE \; p(E) \left[P(E+x) - P(E)\right] (1-P(E))^{M-2}= M \int_{-\infty}^\infty dE \; \left[P(E+x) - P(E)\right] \frac{d Q_{M-1}(E)}{dE} </math></center>
<center><math> \overline{n(x)} = M (M-1) \int_{-\infty}^\infty dE \; p(E) \left[P(E+x) - P(E)\right] (1-P(E))^{M-2}= M \int_{-\infty}^\infty dE \; \left[P(E+x) - P(E)\right] \frac{d Q_{M-1}(E)}{dE} </math></center>


 
where <math>Q_{M-1}(E) = [1-P(E)]^{M-1}</math>.
'''Step 2: the Gumbel limit ''' So far, no approximations have been made. To proceed, we use <math> Q_{M-1}(E)\approx Q_M(E)</math> and its  asymptotics Gumbel form:
'''Step 2: the Gumbel limit ''' So far, no approximations have been made. To proceed, we use <math> Q_{M-1}(E)\approx Q_M(E)</math> and its  asymptotics Gumbel form:

Revision as of 14:10, 31 August 2025

Nei seguente esercizio useremo le notazioni della statistica dei valori estremi usate nel corso.

exercise 1: La distribuzione di Gumbel

esercizio 2: The weakest link

Exercise 3: number of states above the minimum

Definition of :Given a realization of the random energies , define

that is, the number of random variables lying above the minimum but less than . This is itself a random variable. We are interested in its mean value:

The Final goal is to show that for large 'M', when the extremes are described by the Gumbel distribution :

Step 1: Exact manipulations: You start from the exact expression states in the interval:

To compute , you must sum over . Use the identity

to arrive at the form:

where . Step 2: the Gumbel limit So far, no approximations have been made. To proceed, we use and its asymptotics Gumbel form: