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 12:10, 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 n(x):Given a realization of the random energies E1,E2,…,EM, define

n(x)=#{i∣Emin<Ei<Emin+x}

that is, the number of random variables lying above the minimum

Emin

but less than

Emin+x

. This is itself a random variable. We are interested in its mean value:

n(x)‾=∑k=0M−1kProb[n(x)=k]

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

n(x)‾=ex/bM−1

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

Prob[n(x)=k]=M(M−1k)∫−∞∞dEp(E)[P(E+x)−P(E)]k[1−P(E+x)]M−k−1

To compute n(x)‾, you must sum over k. Use the identity

∑k=0M−1k(M−1k)(A−B)kBM−1−k=(A−B)ddA∑k=0M−1(M−1k)(A−B)kBM−1−k=(M−1)(A−B)AM−2

to arrive at the form:

n(x)‾=M(M−1)∫−∞∞dEp(E)[P(E+x)−P(E)](1−P(E))M−2=M∫−∞∞dE[P(E+x)−P(E)]dQM−1(E)dE

where QM−1(E)=[1−P(E)]M−1. Step 2: the Gumbel limit So far, no approximations have been made. To proceed, we use QM−1(E)≈QM(E) and its asymptotics Gumbel form: