PDF see text | CDF see text | |
Support x ∈ ( 0 , c ) {\displaystyle x\in (0,c)\!} Mean μ = c π / 8 χ e − χ 2 4 I 1 ( χ 2 4 ) Ψ ( χ ) {\displaystyle \mu =c{\sqrt {\pi /8}}\;{\frac {\chi e^{-{\frac {\chi ^{2}}{4}}}I_{1}({\tfrac {\chi ^{2}}{4}})}{\Psi (\chi )}}} where I1 is the Modified Bessel function of the first kind of order 1, and Ψ ( x ) {\displaystyle \Psi (x)} is given in the text. Mode c 2 χ ( χ 2 − 2 ) + χ 4 + 4 {\displaystyle {\frac {c}{{\sqrt {2}}\chi }}{\sqrt {(\chi ^{2}-2)+{\sqrt {\chi ^{4}+4}}}}} |
In physics, the ARGUS distribution, named after the particle physics experiment ARGUS, is the probability distribution of the reconstructed invariant mass of a decayed particle candidate in continuum background.
Contents
Definition
The probability density function (pdf) of the ARGUS distribution is:
for 0 ≤ x < c. Here χ, and c are parameters of the distribution and
and Φ(·), ϕ(·) are the cumulative distribution and probability density functions of the standard normal distribution, respectively.
Differential equation
The pdf of the ARGUS distribution is a solution of the following differential equation:
Cumulative distribution function
The cumulative distribution function (cdf) of the ARGUS distribution is
Parameter estimation
Parameter c is assumed to be known (the kinematic limit of the invariant mass distribution), whereas χ can be estimated from the sample X1, …, Xn using the maximum likelihood approach. The estimator is a function of sample second moment, and is given as a solution to the non-linear equation
The solution exists and is unique, provided that the right-hand side is greater than 0.4; the resulting estimator
Generalized ARGUS distribution
Sometimes a more general form is used to describe a more peaking-like distribution:
where Γ(·) is the gamma function, and Γ(·,·) is the upper incomplete gamma function.
Here parameters c, χ, p represent the cutoff, curvature, and power respectively.
The mode is:
p = 0.5 gives a regular ARGUS, listed above.