TBan-I: Difference between revisions
| Line 28: | Line 28: | ||
'''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: | ||
<center><math> | |||
\frac{d Q_{M-1}(E)}{dE} \, dE | |||
\;\sim\; | |||
\exp\!\!\left(\frac{E-a_M}{b_M}\right) | |||
\exp\!\!\left[-\exp\!\!\left(\frac{E-a_M}{b_M}\right)\right] | |||
\frac{dE}{b_M} | |||
= e^{z} e^{-e^{z}} dz | |||
</math></center> | |||
where <math>z = (E-a_M)/b_M</math>. | |||
Revision as of 14:20, 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), you have:
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:
where .