The construction of confidence belts s based on defining horizontal intervals according to a certain confidence level $C$. These can be constructed as central confidence intervals according to

$$ P(x<x_1|\mu)=P(x>x_2|\mu)=(1-C)/2 $$

or as upper confidence limit intervals

$$ P(x<x_1|\mu)=P(x>x_2|\mu)=(1-C)/2 $$

For a given measurement value of $x_0$ these then lead to an interval for $\mu$ with

$$ P(\mu\in[\mu_1,\mu_2])=C $$

This statement means that the unknown true value of $\mu,\mu_t$ lies within the interval $[\mu_1,\mu_2]$ in a fraction $C$ of the experiment conducted

Measurement of a constrained quantity

Bayesian construction with a normalisation that takes the physical limit of $\mu>0$ into account

$$ P(\mu|x)=\frac{e^{-(x-\mu)^2/2\sigma^2}}{\int_0^\infty e^{-(x-\mu')^2/2\sigma^2}d\mu'}(\mu>0) $$

This construction will then lead to one limit being zero, i.e. we set an upper limit

The issue of flip-flopping

❌ Describes choosing between central interval, upper limit etc depending on the measured value. Don’t do this!

The Feldman-Cousins method

it proceeds as follows ( example: Poisson with positive true value and background count $b$ )

Application to Gaussian confidence belts

For a Gaussian (i.e. continuous) variable the procedure is very similar:

🗒️ Note: at $x=1.28$ the distribution transitions from a one-sided to a two sided interval