TBan-I: Difference between revisions
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<center><math> \overline{n(x)} = e^{x/b_M}-1 </math></center> | <center><math> \overline{n(x)} = e^{x/b_M}-1 </math></center> | ||
'''Step 1: Exact manipulations:''' You start from the exact expression | '''Step 1: Exact manipulations:''' You start from the exact expression for the probability of | ||
<math>k</math> states in the interval: | <math>k</math> states in the interval: | ||
<center><math> \text{Prob}[n(x)=k] = M \binom{M-1}{k} \int_{-\infty}^\infty dE \; p(E)\,[P(E+x)-P(E)]^{k}\,[1-P(E+x)]^{M-k-1} </math></center> | <center><math> \text{Prob}[n(x)=k] = M \binom{M-1}{k} \int_{-\infty}^\infty dE \; p(E)\,[P(E+x)-P(E)]^{k}\,[1-P(E+x)]^{M-k-1} </math></center> |
Revision as of 14:11, 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 for the probability of 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: