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| where <math>z = (E-a_M)/b_M</math>. | | where <math>z = (E-a_M)/b_M</math>. |
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| The main contribution to the integral comes from the region near <math>E \approx a_M</math>, where | | The main contribution to the integral comes from the region near <math>E \approx a_M</math>, where <math>P(E) \approx e^{(E-a_M)/b_M}/M</math>. |
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| Compute the integral and verify that you obtain: | | Compute the integral and verify that you obtain: |
Revision as of 14:29, 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
.
The main contribution to the integral comes from the region near
, where
.
Compute the integral and verify that you obtain:
