TBan-I
Detour: Extreme Value Statistics
Consider the 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 M} 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, \dots, E_M} as independent and identically distributed (i.i.d.) random variables drawn from a distribution 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)} . It is useful to introduce the cumulative probability of finding an energy smaller than E
We define:
Our goal is to compute the cumulative distribution:
for large . To achieve this, we rely on three key relations:
- First relation:
This relation is exact but depends on M and the precise form 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 p(E)} . However, in the large M limit, a universal behavior emerges.
- Second relation:
This is an estimation of the typical value of the minimum. It is a crucial relation that will be used frequently in this context.
- Third relation
This is an approximation valid for large M and around the typical value of the minimum energy.