K-distribution
Parameters | {\displaystyle \mu \in (0,+\infty )}, {\displaystyle \alpha \in [0,+\infty )}, {\displaystyle \beta \in [0,+\infty )} | ||
---|---|---|---|
Support | {\displaystyle x\in [0,+\infty )\;} | ||
{\displaystyle {\frac {2}{\Gamma (\alpha )\Gamma (\beta )}},円\left({\frac {\alpha \beta }{\mu }}\right)^{\frac {\alpha +\beta }{2}},円x^{{\frac {\alpha +\beta }{2}}-1}K_{\alpha -\beta }\left(2{\sqrt {\frac {\alpha \beta x}{\mu }}}\right),} | |||
Mean | {\displaystyle \mu } | ||
Variance | {\displaystyle \mu ^{2}{\frac {\alpha +\beta +1}{\alpha \beta }}} | ||
MGF | {\displaystyle \left({\frac {\xi }{s}}\right)^{\beta /2}\exp \left({\frac {\xi }{2s}}\right)W_{-\delta /2,\gamma /2}\left({\frac {\xi }{s}}\right)} |
In probability and statistics, the generalized K-distribution is a three-parameter family of continuous probability distributions. The distribution arises by compounding two gamma distributions. In each case, a re-parametrization of the usual form of the family of gamma distributions is used, such that the parameters are:
- the mean of the distribution,
- the usual shape parameter.
K-distribution is a special case of variance-gamma distribution, which in turn is a special case of generalised hyperbolic distribution. A simpler special case of the generalized K-distribution is often referred as the K-distribution.
Density
[edit ]Suppose that a random variable {\displaystyle X} has gamma distribution with mean {\displaystyle \sigma } and shape parameter {\displaystyle \alpha }, with {\displaystyle \sigma } being treated as a random variable having another gamma distribution, this time with mean {\displaystyle \mu } and shape parameter {\displaystyle \beta }. The result is that {\displaystyle X} has the following probability density function (pdf) for {\displaystyle x>0}:[1]
- {\displaystyle f_{X}(x;\mu ,\alpha ,\beta )={\frac {2}{\Gamma (\alpha )\Gamma (\beta )}},円\left({\frac {\alpha \beta }{\mu }}\right)^{\frac {\alpha +\beta }{2}},円x^{{\frac {\alpha +\beta }{2}}-1}K_{\alpha -\beta }\left(2{\sqrt {\frac {\alpha \beta x}{\mu }}}\right),}
where {\displaystyle K} is a modified Bessel function of the second kind. Note that for the modified Bessel function of the second kind, we have {\displaystyle K_{\nu }=K_{-\nu }}. In this derivation, the K-distribution is a compound probability distribution. It is also a product distribution:[1] it is the distribution of the product of two independent random variables, one having a gamma distribution with mean 1 and shape parameter {\displaystyle \alpha }, the second having a gamma distribution with mean {\displaystyle \mu } and shape parameter {\displaystyle \beta }.
A simpler two parameter formalization of the K-distribution can be obtained by setting {\displaystyle \beta =1} as[2] [3]
- {\displaystyle f_{X}(x;b,v)={\frac {2b}{\Gamma (v)}}\left({\sqrt {bx}}\right)^{v-1}K_{v-1}(2{\sqrt {bx}}),}
where {\displaystyle v=\alpha } is the shape factor, {\displaystyle b=\alpha /\mu } is the scale factor, and {\displaystyle K} is the modified Bessel function of second kind. The above two parameter formalization can also be obtained by setting {\displaystyle \alpha =1}, {\displaystyle v=\beta }, and {\displaystyle b=\beta /\mu }, albeit with different physical interpretation of {\displaystyle b} and {\displaystyle v} parameters. This two parameter formalization is often referred to as the K-distribution, while the three parameter formalization is referred to as the generalized K-distribution.
This distribution derives from a paper by Eric Jakeman and Peter Pusey (1978) who used it to model microwave sea echo.[4] Jakeman and Tough (1987) derived the distribution from a biased random walk model.[5] Keith D. Ward (1981) derived the distribution from the product for two random variables, z = a y, where a has a chi distribution and y a complex Gaussian distribution. The modulus of z, |z|, then has K-distribution.[6]
The moment generating function is given by[7]
- {\displaystyle M_{X}(s)=\left({\frac {\xi }{s}}\right)^{\beta /2}\exp \left({\frac {\xi }{2s}}\right)W_{-\delta /2,\gamma /2}\left({\frac {\xi }{s}}\right),}
where {\displaystyle \gamma =\beta -\alpha ,} {\displaystyle \delta =\alpha +\beta -1,} {\displaystyle \xi =\alpha \beta /\mu ,} and {\displaystyle W_{-\delta /2,\gamma /2}(\cdot )} is the Whittaker function.
The n-th moments of K-distribution is given by[1]
- {\displaystyle \mu _{n}=\xi ^{-n}{\frac {\Gamma (\alpha +n)\Gamma (\beta +n)}{\Gamma (\alpha )\Gamma (\beta )}}.}
So the mean and variance are given by[1]
- {\displaystyle \operatorname {E} (X)=\mu }
- {\displaystyle \operatorname {var} (X)=\mu ^{2}{\frac {\alpha +\beta +1}{\alpha \beta }}.}
Other properties
[edit ]All the properties of the distribution are symmetric in {\displaystyle \alpha } and {\displaystyle \beta .}[1]
Applications
[edit ]K-distribution arises as the consequence of a statistical or probabilistic model used in synthetic-aperture radar (SAR) imagery. The K-distribution is formed by compounding two separate probability distributions, one representing the radar cross-section, and the other representing speckle that is a characteristic of coherent imaging. It is also used in wireless communication to model composite fast fading and shadowing effects.
Notes
[edit ]Sources
[edit ]- Redding, Nicholas J. (1999), Estimating the Parameters of the K Distribution in the Intensity Domain (PDF), South Australia: DSTO Electronics and Surveillance Laboratory, p. 60, DSTO-TR-0839
- Bocquet, Stephen (2011), Calculation of Radar Probability of Detection in K-Distributed Sea Clutter and Noise (PDF), Canberra, Australia: Joint Operations Division, DSTO Defence Science and Technology Organisation, p. 35, DSTO-TR-0839
- Jakeman, Eric; Pusey, Peter N. (1978年02月27日). "Significance of K-Distributions in Scattering Experiments". Physical Review Letters. 40 (9). American Physical Society (APS): 546–550. Bibcode:1978PhRvL..40..546J. doi:10.1103/physrevlett.40.546. ISSN 0031-9007.
- Jakeman, Eric; Tough, Robert J. A. (1987年09月01日). "Generalized K distribution: a statistical model for weak scattering". Journal of the Optical Society of America A. 4 (9). The Optical Society: 1764-1772. Bibcode:1987JOSAA...4.1764J. doi:10.1364/josaa.4.001764. ISSN 1084-7529.
- Ward, Keith D. (1981). "Compound representation of high resolution sea clutter". Electronics Letters. 17 (16). Institution of Engineering and Technology (IET): 561-565. Bibcode:1981ElL....17..561W. doi:10.1049/el:19810394. ISSN 0013-5194.
- Bithas, Petros S.; Sagias, Nikos C.; Mathiopoulos, P. Takis; Karagiannidis, George K.; Rontogiannis, Athanasios A. (2006). "On the performance analysis of digital communications over generalized-k fading channels". IEEE Communications Letters. 10 (5). Institute of Electrical and Electronics Engineers (IEEE): 353–355. CiteSeerX 10.1.1.725.7998 . doi:10.1109/lcomm.2006.1633320. ISSN 1089-7798. S2CID 4044765.
- Long, Maurice W. (2001). Radar Reflectivity of Land and Sea (3rd ed.). Norwood, MA: Artech House. p. 560.
Further reading
[edit ]- Jakeman, Eric (1980年01月01日). "On the statistics of K-distributed noise". Journal of Physics A: Mathematical and General. 13 (1). IOP Publishing: 31–48. Bibcode:1980JPhA...13...31J. doi:10.1088/0305-4470/13/1/006. ISSN 0305-4470.
- Ward, Keith D.; Tough, Robert J. A; Watts, Simon (2006) Sea Clutter: Scattering, the K Distribution and Radar Performance, Institution of Engineering and Technology. ISBN 0-86341-503-2.