TBan-I: Difference between revisions
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In the Gaussian case, expand <math>A(E)</math> around <math>a_M</math>: | In the Gaussian case, expand <math>A(E)</math> around <math>a_M</math>: | ||
By setting | |||
<center><math> | |||
a_M = E_{\min}^{\text{typ}} = -\sigma \sqrt{2 \log M} + \ldots | |||
\qquad\text{and}\qquad | |||
b_M = \frac{1}{A'(a_M)} = \frac{\sigma}{\sqrt{2 \log M}} | |||
</math></center> | |||
you find | |||
Therefore, the variable <math>z = (E - a_M)/b_M</math> is distributed according to an ''M''-independent distribution. | Therefore, the variable <math>z = (E - a_M)/b_M</math> is distributed according to an ''M''-independent distribution. | ||
Revision as of 13:43, 31 August 2025
Nei seguente esercizio useremo le notazioni della statistica dei valori estremi usate nel corso.
Exercise 1: The Gumbel Distribution
In the spirit of the central limit theorem, you look for a scaling form:
The constants and absorb the dependence on , while the random variable is distributed according to a probability distribution that does not depend on .
In the Gaussian case, expand around :
By setting
you find
Therefore, the variable is distributed according to an M-independent distribution.
It is possible to generalize this result and classify the scaling forms into the Gumbel universality class:
- Characteristics:
- Applies when the tails of decay faster than any power law.
- Examples: the Gaussian case discussed here or exponential distributions .
- Scaling Form:
esercizio 2: The weakest link
Exercise 3: number of states above the minimum
Definition of Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle n(x) } :Given a realization of the random energies Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle {E_1, E_2, \ldots, E_M}} , define
that is, the number of random variables lying above the minimum Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle E_{\min}} but less than Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle E_{\min}+x} . 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 Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \overline{n(x)}} , you must sum over Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle k} . Use the identity
to arrive at the form:
where Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle Q_{M-1}(E) = [1-P(E)]^{M-1}} .
Step 2: the Gumbel limit So far, no approximations have been made. To proceed, we use Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle Q_{M-1}(E)\approx Q_M(E)} and its asymptotics Gumbel form:
where Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle z = (E-a_M)/b_M} .
The main contribution to the integral comes from the region near Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle E \approx a_M} , where Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle P(E) \approx e^{(E-a_M)/b_M}/M} .
Compute the integral and verify that you obtain: