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Johnson's SU-distribution
Family of probability distributions
Family of probability distributions
K_{1}=\left( e^{\delta^{-2}} \right)^{2}\left( \left( e^{\delta^{-2}} \right)^{4}+2\left( e^{\delta^{-2}} \right)^{3}+3\left( e^{\delta^{-2}} \right)^{2}-3 \right)\cosh\left( \frac{4\gamma}{\delta} \right) K_2=4\left( e^{\delta^{-2}} \right)^2 \left( \left( e^{\delta^{-2}} \right)+2 \right)\cosh\left( \frac{3\gamma}{\delta} \right) K_3=3\left( 2\left( e^{\delta^{-2}} \right)+1 \right) The Johnson's SU-distribution is a four-parameter family of probability distributions first investigated by N. L. Johnson in 1949. Johnson proposed it as a transformation of the normal distribution:
: z=\gamma+\delta \sinh^{-1} \left(\frac{x-\xi}{\lambda}\right)
where z \sim \mathcal{N}(0,1).
Generation of random variables
Let U be a random variable that is uniformly distributed on the unit interval [0, 1]. Johnson's SU random variables can be generated from U as follows:
: x = \lambda \sinh\left( \frac{ \Phi^{ -1 }( U ) - \gamma }{ \delta } \right) + \xi
where Φ is the cumulative distribution function of the normal distribution.
Johnson's ''SB''-distribution
N. L. Johnson firstly proposes the transformation :
: z=\gamma+\delta \log \left(\frac{x-\xi}{\xi+\lambda-x}\right)
where z \sim \mathcal{N}(0,1).
Johnson's SB random variables can be generated from U as follows: : y={\left(1+{e}^{-\left(z-\gamma\right) /\delta }\right)}^{-1} : x=\lambda y +\xi
The SB-distribution is convenient to Platykurtic distributions (Kurtosis). To simulate SU, sample of code for its density and cumulative distribution function is available here
Applications
Johnson's S_{U}-distribution has been used successfully to model asset returns for portfolio management. This comes as a superior alternative to using the Normal distribution to model asset returns. An R package, JSUparameters, was developed in 2021 to aid in the estimation of the parameters of the best-fitting Johnson's S_{U}-distribution for a given dataset. Johnson distributions are also sometimes used in option pricing, so as to accommodate an observed volatility smile; see Johnson binomial tree.
An alternative to the Johnson system of distributions is the quantile-parameterized distributions (QPDs). QPDs can provide greater shape flexibility than the Johnson system. Instead of fitting moments, QPDs are typically fit to empirical CDF data with linear least squares.
Johnson's S_{U}-distribution is also used in the modelling of the invariant mass of some heavy mesons in the field of B-physics.
References
References
- Johnson, N. L.. (1949). "Systems of Frequency Curves Generated by Methods of Translation". [[Biometrika]].
- Johnson, N. L.. (1949). "Bivariate Distributions Based on Simple Translation Systems". [[Biometrika]].
- Tsai, Cindy Sin-Yi. (2011). "The Real World is Not Normal". Morningstar Alternative Investments Observer.
- LHCb Collaboration. (2022). "Precise determination of the – oscillation frequency". Nature Physics.
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